Interaction of ions and water in gramicidin A channels: streaming potentials across lipid bilayer membranes

For very narrow channels in which ions and water cannot overtake one another (single-file transport), electrokinetic measurements provide information about the number of water molecules within a channel. Gramicidin A is believed to form such narrow channels in lipid bilayer membranes. In 0.01 and 0.1 M solutions of CsCl, KCL, and NaCl, streaming potentials of 3.0 mV per osmolal osmotic pressure difference (created by urea, glycerol, or glucose) appear across gramicidin A-treated membranes. This implies that there are six to seven water molecules within a gramicidin channel. Electroosmotic experiments, in which the water flux assoicated with current flow across gramicidin-treated membranes is measured, corroborate this result. In 1 M salt solutions, streaming potentials are 2.35 mV per osmolal osmotic pressure difference instead of 3.0 mV. The smaller value may indicate multiple ion occupancy of the gramicidin channel at high salt concentrations. Apparent deviations from ideal cationic selectivity observed while attempting to measure single-salt dilution potentials across gramicidin-treated membranes result from streaming potential effects.     

Fusion of phospholipid vesicles with planar phospholipid bilayer membranes. II. Incorporation of a vesicular membrane marker into the planar membrane

Fusion of multilamellar phospholipid vesicles with planar phospholipid bilayer membranes was monitored by the rate of appearance in the planar membrane of an intrinsic membrane protein present in the vesicle membranes. An essential requirement for fusion is an osmotic gradient across the planar membrane, with the cis side (the side containing the vesicles) hyperosmotic to the opposite (trans) side; for substantial fusion rates, divalent cation must also be present on the cis side. Thus, the low fusion rates obtained with 100 mM excess glucose in the cis compartment are enhanced orders of magnitude by the addition of 5-10 mM CaCl2 to the cis compartment. Conversely, the rapid fusion rates induced by 40 mM CaCl2 in the cis compartment are completely suppressed when the osmotic gradient (created by the 40 mM CaCl2) is abolished by addition of an equivalent amount of either CaCl2, NaCl, urea, or glucose to the trans compartment. We propose that fusion occurs by the osmotic swelling of vesicles in contact with the planar membrane, with subsequent rupture of the vesicular and planar membranes in the region of contact. Divalent cations catalyze this process by increasing the frequency and duration of vesicle-planar membrane contact. We argue that essentially this same osmotic mechanism drives biological fusion processes, such as exocytosis. Our fusion procedure provides a general method for incorporating and reconstituting transport proteins into planar phospholipid bilayer membranes.     

The cell wall porin of the gram-positive bacterium Nocardia asteroides forms cation-selective channels that exhibit asymmetric voltage dependence

Detergent-solubilized cell wall extracts of the gram-positive, strictly aerobic bacterium Nocardia asteroides contain channel-forming activity as judged from reconstitution experiments using lipid bilayer membranes. The cell wall porin was identified as a protein with an apparent molecular mass of about 84 kDa based on SDS-PAGE. The porin was purified to homogeneity using preparative SDS-PAGE. The 84-kDa protein was no longer observed after heating in SDS buffer. The presumed dissociation products were not observed on SDS-polyacrylamide gels. The cell wall porin increased the specific conductance of artificial lipid bilayer membranes from phosphatidylcholine/phosphatidylserine mixtures by the formation of cation-selective channels, which had an average single-channel conductance of 3.0 nS in 1 M KCl. The single-channel conductance was only moderately dependent on the bulk aqueous KCl concentration, which indicated negative point charge effects on the channel properties. The analysis of the concentration dependence of the single-channel conductance using the effect of negative charges on channel conductance suggested that the diameter of the cell wall channel is about 1.4 nm. Asymmetric addition of the cell wall porin to lipid bilayer membranes resulted in an asymmetric voltage dependence. The cell wall channel switched into substates, when the cis side of the membrane, the side of the addition of the protein, had negative polarity. Positive potentials at the cis side had no influence on the conductance of the cell wall channel. Received: 23 September 1998 / Accepted: 9 December 1998     

Coupling of water and potassium ions in K+ channels of the tonoplast of Chara

Electrokinetic measurements, of streaming potential, were carried out on an excised inside-out patch of the vacuolar membrane of Chara corallina. A water activity gradient was imposed across the patch membrane containing a single K⁺ channel by addition of sorbitol to one side. Two different K⁺ channels were found in the tonoplast. Their open channel conductance was investigated as a function of KCl concentration. They had a maximal open channel conductance of 247 and 173 pS, and an apparent affinity (K_M) of 116 and 92 mM, respectively. Single-channel zero-current potentials were determined in the presence of an osmotic gradient, and dilution artifacts were corrected for by addition of valinomycin to the bath. Our results suggest that 29 water molecules were coupled to the transport of one K⁺ ion in the large conductance K⁺ channel which has a pore radius of ~1.5 nm.     

Streaming potential measurements in Ca2+-activated K+ channels from skeletal and smooth muscle. Coupling of ion and water fluxes.

Streaming potentials arising across large-conductance Ca2+-activated K+ channels incorporated into planar lipid bilayers were measured. Ca2+-activated channels obtained either from skeletal muscle or from smooth muscle membranes were used. Streaming potentials were extracted from the current-voltage relationship for the open channel obtained in the presence of an osmotic gradient. The osmotic gradient was established by adding glucose to one side of the membrane. At 300 mM KCl, the average streaming potential was 0.72 mV/osmol per kg for t-tubule channels and 0.83 mV/osmol per kg for smooth muscle channels. Streaming potential values depend on KCl concentration, they decrease as KCl concentration increases, and the value obtained by extrapolation to zero KCl concentration is 0.85 mV/osmol per kg. Assuming that water and ions cannot pass each other, at least in a region of the channel, the streaming potential values obtained indicate that this region contains a minimum of two and a maximum of four water molecules. It is concluded that the channel has a narrow region with a length of 0.6-1.2 nm.     

Parameters affecting the fusion of unilamellar phospholipid vesicles with planar bilayer membranes

It was previously shown (Cohen, F. S., J. Zimmerberg, and A. Finkelstein, 1980, J. Gen. Physiol., 75:251-270) that multilamellar phospholipid vesicles can fuse with decane-containing phospholipid bilayer membranes. An essential requirement for fusion was an osmotic gradient across the planar membrane, with the vesicle-containing (cis) side hyperosmotic with respect to the opposite (trans) side. We now report that unilamellar vesicles will fuse with "hydrocarbon-free" membranes subject to these same osmotic conditions. Thus the same conditions that apply to fusion of multilamellar vesicles with planar bilayer membranes also apply to fusion of unilamellar vesicles with these membranes, and hydrocarbon is not required for the fusion process. If the vesicles and/or planar membrane contain negatively charged lipids, divalent cation (approximately 15 mM Ca++) is required in the cis compartment (in addition to the osmotic gradient across the membrane) to obtain substantial fusion rates. On the other hand, vesicles made from uncharged lipids readily fuse with planar phosphatidylethanolamine planar membranes in the near absence of divalent cation with just an osmotic gradient. Vesicles fuse much more readily with phosphatidylethanolamine-containing than with phosphatidylcholine-containing planar membranes. Although hydrocarbon (decane) is not required in the planar membrane for fusion, it does affect the rate of fusion and causes the fusion process to be dependent on stirring in the cis compartment.     

Probing membrane permeabilization by the antimicrobial peptide distinctin in mercury-supported biomimetic membranes

The mechanism of membrane permeabilization by the antimicrobial peptide distinctin was investigated by using two different mercury-supported biomimetic membranes, namely a lipid self-assembled monolayer and a lipid bilayer tethered to the mercury surface through a hydrophilic spacer (tethered bilayer lipid membrane: tBLM). Incorporation of distinctin into a lipid monolayer from its aqueous solution yields rapidly ion channels selective toward inorganic cations, such as Tl(+) and Cd(2+). Conversely, its incorporation in a tBLM allows the formation of ion channels permeable to potassium ions only at non-physiological transmembrane potentials, more negative than -340mV. These channels, once formed, are unstable at less negative transmembrane potentials. The kinetics of their formation is consistent with the disruption of distinctin clusters adsorbed on top of the lipid bilayer, incorporation of the resulting monomers and their aggregation into hydrophilic pores by a mechanism of nucleation and growth. Comparing the behavior of distinctin in tBLMs with that in conventional black lipid membranes strongly suggests that distinctin channel formation in lipid bilayer requires the partitioning of distinctin molecules between the two sides of the lipid bilayer. We can tentatively hypothesize that an ion channel is formed when one distinctin cluster on one side of the lipid bilayer matches another one on the opposite side.     

Fusion of phospholipid vesicles with a planar membrane depends on the membrane permeability of the solute used to create the osmotic pressure

Phospholipid vesicles fuse with a planar membrane when they are osmotically swollen. Channels in the vesicle membrane are required for swelling to occur when the vesicle-containing compartment is made hyperosmotic by adding a solute (termed an osmoticant). We have studied fusion using two different channels, porin, a highly permeable channel, and nystatin, a much less permeable channel. We report that an osmoticant's ability to support fusion (defined as the magnitude of osmotic gradient necessary to obtain sustained fusion) depends on both its permeability through lipid bilayer as well as its permeability through the channel by which it enters the vesicle interior. With porin as the channel, formamide requires an osmotic gradient about ten times that required with urea, which is approximately 1/40th as permeant as formamide through bare lipid membrane. When nystatin is the channel, however, fusion rates sustained by osmotic gradients of formamide are within a factor of two of those obtained with urea. Vesicles containing a porin-impermeant solute can be induced to swell and fuse with a planar membrane when the impermeant bathing the vesicles is replaced by an isosmotic quantity of a porin-permeant solute. With this method of swelling, formamide is as effective as urea in obtaining fusion. In addition, we report that binding of vesicles to the planar membrane does not make the contact region more permeable to the osmoticant than is bare lipid bilayer. In the companion paper, we quantitatively account for the observation that the ability of a solute to promote fusion depends on its permeability properties and the method of swelling. We show that the intravesicular pressure developed drives fusion.     

TonB-Dependent Transporter FhuA in Planar Lipid Bilayers: Partial Exit of Its Plug from the Barrel

TonB-dependent transporters (TBDTs), which transport iron-chelating siderophores and vitamin B(12) across the outer membrane of Gram-negative bacteria, share a conserved architecture of a 22-stranded β-barrel with an amino-terminal plug domain occluding the barrel. We previously reported that we could induce TBDTs to reversibly open in planar lipid bilayers via the use of urea and that these channels were responsive to physiological concentrations of ligands. Here we report that in the presence of urea, trypsin can cleave the amino-terminal 67 residues of the plug of the TonB-dependent transporter FhuA, as assessed by gel shift and mass spectrometry assays. On the bilayer, trypsin treatment in the presence of urea resulted in the induced conductance no longer being reversed upon removal of urea, suggesting that urea opens intact FhuA channels by pulling the plug at least partly out of the barrel and that removal of the urea then allows reinsertion of the plug into the barrel. When expressed separately, the FhuA plug domain was found to be a mostly unfolded structure that was able to occlude isolated FhuA β-barrels inserted into the membrane. Thus, although folded in the barrel, the plug need not be folded upon exiting the barrel. The rate of insertion of the β-barrels into the membrane was tremendously increased in the presence of an osmotic gradient provided by either urea or glycerol. Negative staining electron microscopy showed that FhuA in a detergent solution formed vesicles, thus explaining why an osmotic gradient promoted the insertion of FhuA into membranes.     

Characterization of diphtheria toxin-induced lesions in liposomal membranes. An evaluation of the relationship between toxin insertion and "channel" formation

Diphtheria toxin interaction with membranes has been studied by following the release of a fluorescent dye (calcein) encapsulated within large unilamellar vesicles. Results showed that diphtheria toxin induced temperature- as well as pH-dependent permeability changes in these model membranes. Interestingly, insertion of the "channel-forming" B domain was not sufficient for calcein release, since dye release from vesicles composed of dimyristoyllecithin:cholesterol:dicetylphosphate 4:3:0.8) was completely inhibited at low temperatures which permitted B insertion. Rather, the temperature dependence of calcein release from and A domain insertion into dimyristoyllecithin:cholesterol:dicetyl phosphate vesicles suggest some relationship between "channel formation" and fragment A translocation across membranes. However, the nature of the toxin channel is called into question by our observations that channel size, in addition to activity, was pH-dependent. On the basis of these experiments, it is proposed that the toxin "channel" is the result of localized perturbations in the lipid bilayer at the interface between lipids and inserted toxin molecules that are sufficiently large in fluid membranes at low pH to allow the translocation of fragment A across the bilayer.     

The peptaibol antiamoebin as a model ion channel: similarities to bacterial potassium channels.

Antiamoebin (AAM) is a polypeptide antibiotic that is capable of forming ion channels in phospholipid membranes: planar bilayer studies have suggested the channels are octamers. The crystal structure of a monomeric form of AAM has provided the basis for molecular modelling of an octameric helical bundle channel. The channel model is funnel-shaped due to a substantial bend in the middle of the polypeptide chain caused by the presence of several imino acids. Inter-monomer hydrogen bonds orientate a ring of glutamine side chains to form a constriction in the pore lumen. The channel lumen is lined both by side chains of Gln11 and by polypeptide backbone carbonyl groups. Electrostatic calculations on the model are compatible with a channel that transports cations across membranes. The AAM channel model is compared with the crystal structures of two bacterial (KcsA andMthK) potassium channels. AAM and the potassium channels exhibit common functional features, such as cation-selectivity and similar single channel conductances. Common structural features include being multimers, each formed from a bundle of eight transmembrane helices, with lengths roughly comparable to the thickness of lipid bilayers. In addition, they all have aromatic amino acids that lie at the bilayer interfaces and which may aid in the stabilization of the transmembrane helices, as well as narrower constrictions that define the ion binding sites or selectivity filters in the pore lumen. The commonality of structural and functional features in these channels thus suggests that antiamoebin is a good, simple model for more complex bacterial and eukaryotic ion channels, capable of providing insight into details of the mechanisms of ion transport and multimeric channel stability.     

Role of channels in the fusion of vesicles with a planar bilayer.

Fluorescence microscopy combined with electrical conductance measurements were used to assess fusion of phospholipid vesicles with a planar bilayer. Large unilamellar vesicles (0.5-3 microns diam.) filled with the fluorescent dye, calcein, were made both with or without porin channels. Vesicle-bilayer fusion was induced by increasing the osmolarity of the solution on the side of the bilayer to which the vesicles were added. Fusion was detected optically by the fluorescent flash due to release of vesicular contents. Although both porin-containing and porin-free vesicles give the same kind of flash upon content release, the conditions necessary to induce release are very different. Only 4% of the porin-free vesicles fuse (release their contents) when subjected to 3 M urea. However, the same conditions induce 53% of the porin-containing vesicles to fuse and most of these fusions occur at a lower osmolarity ([urea] less than 400 mM). Thus channels greatly enhance fusion in this model system. A physical model based on the postulate that fusion is induced by an increase in surface tension, predicts that three conditions are necessary for fusion in this system: (a) an open channel in the vesicle membrane, (b) an osmotic gradient across the bilayer, and (c) the vesicle in contact with the planar membrane. These are the conditions that experimentally produce fusion in the model system.     

Osmotic regulation of assimilate unloading from seed coats of Vicia faba. Role of turgor and identification of turgor-dependent fluxes

Osmotic regulation of assimilate efflux from excised coats of developing Vicia faba (cv. Coles Prolific) seed was examined by exposing these to bathing solutions (adjusted to –0. 02 to –0. 75 MPa with sorbitol) introduced into the cavity vacated by the embryo. ¹⁴C photosynthate efflux was found to be independent of solution osmotic potentials below –0. 63 MPa. At higher osmotic potentials, efflux was stimulated and exhibited a biphasic response to osmotic potential with apparent saturation being reached at –0. 37 MPa. Efflux could be repeatedly stimulated and slowed by exposing seed coats to solutions of high and low osmotic potentials, respectively. Manipulation of components of tissue water potential, with slowly- and rapidly-permeating osmotica, demonstrated that turgor functioned as the signal regulating ¹⁴C photosynthate efflux. Com-partmental analysis of ¹⁴C photosynthate preloaded seed coats was consistent with exchange from 4 kinetically-distinct compartments. The kinetics of turgor-dependent efflux exhibited characteristics consistent with the transport mechanism residing in the plasma membranes of the unloading cells. These characteristics included the rapidity (<2 min) of the efflux response to turgor increases, similar rate constants for efflux from the putative turgor-sensitive and cytoplasmic compartments and the apparent small pool size from which turgor-dependent efflux could repeatedly occur. In contrast, influx of [¹⁴C] sucrose across the plasma and tonoplast membranes was found to be insensitive to turgor. The plasma membrane [¹⁴C] sucrose influx was unaffected by p-chloromercuribenzenesulfonic acid and erythrosin B and exhibited a linear dependence on the external sucrose concentration. This behaviour suggested that influx across the plasma membrane occurs by passive diffusion. Preloading excised seed coats with a range of solutes demonstrated that turgor-dependent efflux exhibited partial solute selectivity. Based on these findings, it is proposed that turgor controls assimilate exchange from the seed coat by regulating an efflux mechanism located in the plasma membranes of the unloading cells.     

Translocation and interactions of L-arabinose in OmpF porin: A molecular dynamics study

The passage of a natural substrate, L-arabinose (L-ARA) through Escherichia coli porin embedded in an artificial bilayer, is studied by equilibrium molecular dynamics simulations. We investigate the early stage of translocation process of L-ARA from intra-cellular to extra-cellular side (Int-to-Ext) across the bilayer. The average trajectory path over all L-ARA molecules along with quantum-mechanical configuration-optimizations at PM3 level predict the existence of at least three trapping zones. The common feature within all these zones is that L-ARA remains perpendicular to the channel axis. It is remarkable how the orientation and translational-rotational motion of L-ARA molecule play a role in its transport through OmpF channel. These simulations are important for better understanding of permeation process in OmpF channel. They also provide an insight into the chiral recognition of translocation process in protein nanochannels from substrate and protein prospects and help interpret experiments on permeation process of small dipolar molecules across biological membranes.     

Major transmembrane movement associated with colicin Ia channel gating

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

Cluster organization of ion channels formed by the antibiotic syringomycin E in bilayer lipid membranes.

The cyclic lipodepsipeptide, syringomycin E, when incorporated into planar lipid bilayer membranes, forms two types of channels (small and large) that are different in conductance by a factor of sixfold. To discriminate between a cluster organization-type channel structure and other possible different structures for the two channel types, their ionic selectivity and pore size were determined. Pore size was assessed using water-soluble polymers. Ion selectivity was found to be essentially the same for both the small and large channels. Their reversal (zero current) potentials with the sign corresponding to anionic selectivity did not differ by more than 3 mV at a twofold electrolyte gradient across the bilayer. Reduction in the single-channel conductance induced by poly(ethylene glycol)s of different molecular weights demonstrated that the aqueous pore sizes of the small and large channels did not differ by more than 2% and were close to 1 nm. Based on their virtually identical selectivity and size, we conclude that large syringomycin E channels are clusters of small ones exhibiting synchronous opening and closing.     

Do Trehalose and Dimethyl Sulfoxide Affect Intermembrane Forces?

The sugar trehalose is produced in some organisms that survive dehydration and desiccation, and it preserves the integrity of membranes in model systems exposed to dehydration and freezing. Dimethyl sulfoxide, a solute which permeates membranes, is added to cell suspensions in many protocols for cryopreservation. Using a surface forces apparatus, we measured the very large, short-range repulsion between phosphatidylcholine bilayers in water and in solutions of trehalose, sorbitol, and dimethyl-sulfoxide. To the resolution of the technique, the force-distance curves between bilayers are unchanged by the addition of trehalose or sorbitol in concentrations exceeding 1 kmol · m^-3. A relatively small increase in adhesion in the presence of trehalose and sorbitol solutions may be explained by their osmotic effects. The partitioning of trehalose between aqueous solutions and lamellar phases of dioleylphosphatidylcholine was measured gravimetrically. The amount of trehalose that preferentially adsorbs near membrane surfaces is at most small. The presence of dimethyl sulfoxide in water ( 1:2 by volume) makes very little difference to the short-range interaction between deposited bilayers, but it sometimes perturbs them in ways that vary among experiments: free bilayers and/or fusion of the deposited bilayers were each observed in about one-third of the experiments.     

Aquaporin Membrane Channels: Biophysics, Classification, Functions, and Possible Biotechnological Applications

Water represents the major component of all living organisms. To make the cell to adapt to the surrounding environment and carry out its biological functions, water has to move into and out of the cell interior driven by osmotic forces. For over a century, scientists studying the movement of fluid into and out of the cell struggled with a difficult biophysical question: how does water pass through the cell? Movement of water across the membrane was indicated almost as soon as the lipid bilayer was recognized as being the plasma membrane of cells, back in the 1920s. Simple diffusion of water across the lipid bilayer occurs through all biological membranes. However, its low velocity and finite extent soon became apparent, suggesting the existence of additional pathways for water moving through the membrane. In spite of the enormous amount of work carried out in this area, the precise and complete answer only came relatively recently with the discovery of aquaporins, transmembrane channel proteins making the membrane tenfold to 100-fold more permeable to water than membranes lacking such pores. The water conductance featured by the aquaporins is astonishing: in fact, each single aquaporin pore can conduct billions of water molecules per second. A branch of the aquaporin family, the aquaglyceroporins, features conductance to small neutral solutes in addition to water. This review summarizes recent updates on the molecular structure, regulation, biophysics, and biological functions of aquaporins. Possible biotechnological applications of aquaporins are also described.     

Pore formation by the Bordetella adenylate cyclase toxin in lipid bilayer membranes: role of voltage and pH

The bifunctional adenylate cyclase toxin (ACT or CyaA) of Bordetella pertussis invades target cells via transport through the cytoplasmic membrane. The membrane potential represents thereby an important factor for the uptake in vivo. Previous studies demonstrated that adenylate cyclase (AC) delivery into cells requires a negative membrane potential inside the cells. The results of lipid bilayer experiments with ACT presented here indicated that two different types of pore-like structures are formed by ACT dependent on the orientation of the electrical potential across the membranes. Pore formation at a positive potential at the cis side of the membranes, the side of the addition of the toxin, was fast and its conductance had a defined size, whereas at negative potential the pores were not defined, had a reduced pore-forming activity and a very short lifetime. Fluctuations inserted at positive potentials showed asymmetric current-voltage relationships for positive and negative voltages. Positive potentials at the cis side resulted in an increasing current, whereas at negative potentials the current decreased or remained at a constant level. Calcium ions enhanced the voltage dependence of the ACT pores when they were added to the cis side. The single-pore conductance was strongly affected by the variation of the pH value and increased in 1M KCl with increasing pH from about 4 pS at pH 5 to about 60 pS at pH 9. The ion selectivity remained unaffected by pH. Experiments with ACT mutants revealed, that the adenylate cyclase (AC) and repeat (RT) domains were not involved in voltage and pH sensing.     

Pore formation by the Bordetella adenylate cyclase toxin in lipid bilayer membranes: Role of voltage and pH

The bifunctional adenylate cyclase toxin (ACT or CyaA) of Bordetella pertussis invades target cells via transport through the cytoplasmic membrane. The membrane potential represents thereby an important factor for the uptake in vivo. Previous studies demonstrated that adenylate cyclase (AC) delivery into cells requires a negative membrane potential inside the cells. The results of lipid bilayer experiments with ACT presented here indicated that two different types of pore-like structures are formed by ACT dependent on the orientation of the electrical potential across the membranes. Pore formation at a positive potential at the cis side of the membranes, the side of the addition of the toxin, was fast and its conductance had a defined size, whereas at negative potential the pores were not defined, had a reduced pore-forming activity and a very short lifetime. Fluctuations inserted at positive potentials showed asymmetric current-voltage relationships for positive and negative voltages. Positive potentials at the cis side resulted in an increasing current, whereas at negative potentials the current decreased or remained at a constant level. Calcium ions enhanced the voltage dependence of the ACT pores when they were added to the cis side. The single-pore conductance was strongly affected by the variation of the pH value and increased in 1M KCl with increasing pH from about 4 pS at pH 5 to about 60 pS at pH 9. The ion selectivity remained unaffected by pH. Experiments with ACT mutants revealed, that the adenylate cyclase (AC) and repeat (RT) domains were not involved in voltage and pH sensing.