Influenza hemagglutinin-mediated fusion pores connecting cells to planar membranes: flickering to final expansion

We have studied the fusion between voltage-clamped planar lipid bilayers and influenza virus infected MDCK cells, adhered to one side of the bilayer, using measurements of electrical admittance and fluorescence. The changes in currents in-phase and 90 degrees out-of- phase with respect to the applied sinusoidal voltage were used to monitor the addition of the cell membrane capacitance to that of the lipid bilayer through a fusion pore connecting the two membranes. When ethidium bromide was included in the solution of the cell-free side of the bilayer, increases in cell fluorescence accompanied tee admittance changes, independently confirming that these changes were due to formation of a fusion pore. Fusion required acidic pH on the cell- containing side and depended on temperature. For fusion to occur, the influenza hemagglutinin (HA) had to be cleaved into HA1 and HA2 subunits. The incorporation of gangliosides into the planar bilayers greatly augmented fusion. Fusion pores developed in four distinct stages after acidification: (a) a pre-pore, electrically quiescent stage; (b) a flickering stage, with 1-2 nS pores opening and closing repetitively; (c) an irreversibly opened stage, in which pore conductances varied between 2 and 100 nS and exhibited diverse kinetics; (d) a fully opened stage, initiated by an instantaneous, time- resolution limited, increase in conductance leveling at approximately 500 nS. The expansion of pores by stages has also been shown to occur during exocytosis in mast cells and fusion of HA-expressing cells and erythrocytes. We conclude that essential features of fusion pores are produced with proteins in just one of the two fusing membranes.     

The initial fusion pore induced by baculovirus GP64 is large and forms quickly

The formation of the fusion pore is the first detectable event in membrane fusion (Zimmerberg, J., R. Blumenthal, D.P. Sarkar, M. Curran, and S.J. Morris. 1994. J. Cell Biol. 127:1885-1894). To date, fusion pores measured in exocytosis and viral fusion have shared features that include reversible closure (flickering), highly fluctuating semistable stages, and a lag time of at least several seconds between the triggering and the pore opening. We investigated baculovirus GP64- induced Sf9 cell-cell fusion, triggered by external acid solution, using two different electrophysiological techniques: double whole-cell recording (for high time resolution, model-independent measurements), and the more conventional time-resolved admittance recordings. Both methods gave essentially the same results, thus validating the use of the admittance measurements for fusion pore conductance calculations. Fusion was first detected by abrupt pore formation with a wide distribution of initial conductance, centered around 1 nS. Often the initial fusion pore conductance was stable for many seconds. Fluctuations in semistable conductances were much less than those of other fusion pores. The waiting time distribution, measured between pH onset and initial pore appearance, fits best to a model with many (approximately 19) independent elements. Thus, unlike previously measured fusion pores, GP64-mediated pores do not flicker, can have large, stable initial pore conductances lasting up to a minute, and have typical lag times of < 1 s. These findings are consistent with a barrel-shaped model of an initial fusion pore consisting of five to eight GP64 trimers that is lined with lipid.     

Patch clamp studies of single intact secretory granules.

The membrane of secretory granules is involved in the molecular events that cause exocytotic fusion. Several of the proteins that have been purified from the membrane of secretory granules form ion channels when they are reconstituted in lipid bilayers and, therefore, have been thought to form part of the molecular structure of the exocytotic fusion pore. We have used the patch clamp technique to study ion conductances in single isolated secretory granules from beige mouse mast cells. We found that the membrane of the intact granule had a conductance of < 50 pS. No abrupt changes in current corresponding to the opening and closing of ion channels were observed, even under conditions where exocytotic fusion occurred. However, mechanical tension or a large voltage pulse caused the breakdown of the granule membrane resulting in the abrupt opening of a pore with an ion conductance of about 1 nS that fluctuated rapidly and could expand to an immeasurably large conductance or close completely. Surprisingly, the behavior of these pores resembled the pattern of conductance changes of exocytotic fusion pores observed in degranulating beige mast cells. This similarity supports the view that the earliest fusion pore is formed upon the breakdown of a bilayer such as that formed during hemifusion.     

Hemagglutinin-induced fusion of HAb2 and PLC cells: dynamics of fusion pore conductance

Infection of cells with influenza virus is mediated by the virus envelope protein hemagglutinin (HA) which induces fusion of viral and target membranes. Earlier we showed using fluorescent microscopy that HAb2 cells expressing HA on their plasma membranes fused with PLC cells when pH of the external medium was decreased to -5. In the present work we used double whole-cell recording to monitor the intercellular conductance in HAb2/PLC cell pairs during fusion. In approximately 40% of cell pairs the pH drop induced the intercellular conductance, which we interpret as the formation of a fusion pore. The following stages of the conductance growth were distinguished: initial fluctuations near zero (flicker), a subsequent slow increase up to 1-4 nS and a final rapid increase up to 10-100 nS (complete fusion). The first detectable intercellular conductance change (opening of a fusion pore) was accompanied by an increase in the conductances of both HAb2 and PLC cell membrane. This observation suggests that the early pore complex should be leaky. The dynamics of the intercellular conductance appeared to depend upon the voltage difference between the fusing HAb2 and PLC cells: voltages higher than 40 mV facilitated the conductance growth.     

Exocytotic fusion pores exhibit semi-stable states

Summary Rapid-freezing/freeze-fracture electron microscopy and whole-cell capacitance techniques were used to study degranulation in peritoneal mast cells of the rat and the mutant beige mouse. These studies allowed us to create a time-resolved picture for fusion pore formation. After stimulation, a dimple in the plasma membrane formed a small contact area with the secretory granule membrane. Within this zone of apposition no ordered proteinaceous specializations were seen. Electrophysiological technique measured a small fusion pore which widened rapidly to 1 nS. Thereafter, the fusion pore remained at semi-stable conductances between 1 and 20 nS for a wide range of times, between 10 and 15,000 msec. These conductances correspond to pore diameters 25–36 nm. Ultrastructural data confirmed small pores of hourglass morphology, composed of biological membrane coplanar with both the plasma and granular membranes. Later, the fusion pore rapidly increased in conductance, consistent with the observed morphology of omega-figures. The hallmarks of channel-like behavior, instantaneous jumps in pore conductance between defined levels, and sharp peaks in histograms of conductance dwell-time, were not seen. Since the morphology of small pores shows contiguous fracture planes, the electrical data represent pores that contain lipid. These combined morphological and electrophysiological data are consistent with a lipid/protein complex mediating both the initial and later stages of membrane fusion.We would like to dedicate this paper to the memory of our friend and mentor, Alex Mauro, who emphasized to us the importance of equivalent circuits. This work was supported by National Institutes of Health grant GM-27367, and National Science Foundation grant IBN-91117509.     

Large cation-selective pores from rat liver peroxisomal membranes incorporated to planar lipid bilayers

Summary Fusion of a highly purified fraction of rat liver peroxisomal membranes to planar lipid bilayers incorporates large, cation-selective voltage-dependent pores. TheP _K/P _Cl ratio of these pores, estimated in KCl gradients, is close to 4. The pores display several conductance states and spend most of the time open at voltages near 0 mV, closing at more positive and negative voltages. At voltages near 0 mV the most frequent open state has a conductance of 2.4 nS in 0.3m KCl. At voltages more positive and more negative than 10 mV the most frequent open state displays a conductance of 1.2 nS in 0.3m KCl. With these results pore diameters of 3 and 1.5 nm, respectively, can be estimated. We suggest that these pores might account for the unusually high permeability of peroxisomes to low molecular weight solutes. Fusion also incorporates a perfectly anion-selective, two-open states channel with conductances of 50 and 100 pS in 0.1m KCl.     

Membrane flux through the pore formed by a fusogenic viral envelope protein during cell fusion

We have investigated the mechanism of cell fusion mediated by HA, the fusogenic hemagglutinin of the Influenza viral envelope. Single erythrocytes (RBCs) were attached to fibroblasts expressing the HA on their cell surface, and fusion of the paired cells was triggered by rapid acidification. The RBC membrane was stained with fluorescent lipid, and the fusion-induced escape of lipid into the fibroblast was observed by quantitative image analysis. At the same time, the formation of an aqueous connection (i.e., the fusion pore) between the two cells was monitored electrically. Within minutes after acidification, an electrical conductance between the two cells appeared abruptly as the fusion pore opened, and then increased gradually as the pore dilated. Later, fluorescent lipid diffused into the fibroblast, approaching equilibrium over the next 5-20 min. No lipid flux was seen while the pore conductance remained 0.5 nS or less. Evidently lipid flux requires a threshold pore size. Our finding suggests that the smallest and earliest fusion pores are surrounded by a ring of protein. A fusion pore expands by breaking this ring and recruiting lipid into its circumference.     

Voltage-induced nonconductive pre-pores and metastable single pores in unmodified planar lipid bilayer

Electric fields promote pore formation in both biological and model membranes. We clamped unmodified planar bilayers at 150-550 mV to monitor transient single pores for a long period of time. We observed fast transitions between different conductance levels reflecting opening and closing of metastable lipid pores. Although mean lifetime of the pores was 3 +/- 0.8 ms (250 mV), some pores remained open for up to approximately 1 s. The mean amplitude of conductance fluctuations (approximately 500 pS) was independent of voltage and close for bilayers of different area (40,000 and 10 microm(2)), indicating the local nature of the conductive defects. The distribution of pore conductance was rather broad (dispersion of approximately 250 pS). Based on the conductance value and its dependence of the ion size, the radius of the average pore was estimated as approximately 1 nm. Short bursts of conductance spikes (opening and closing of pores) were often separated by periods of background conductance. Within the same burst the conductance between spikes was indistinguishable from the background. The mean time interval between spikes in the burst was much smaller than that between adjacent bursts. These data indicate that opening and closing of lipidic pores proceed through some electrically invisible (silent) pre-pores. Similar pre-pore defects and metastable conductive pores might be involved in remodeling of cell membranes in different biologically relevant processes.     

Influenza virus hemagglutinin-induced cell-planar bilayer fusion: quantitative dissection of fusion pore kinetics into stages

Cells expressing the influenza virus hemagglutinin (HA) fuse to planar bilayer membranes under acidic conditions. After an electrically quiescent perfusion stage (Q), a fusion pore forms that enlarges in three subsequent stages. A repetitively flickering pore stage (R) develops into a securely open stage (S) that exhibits conductances ranging from a few to tens of nS. The pore then expands to a terminal stage (T) with a large conductance on the order of one microSiemens. We have studied how virus strain, HA receptors in the target bilayer membrane, and cytoskeleton affect the time a fusion pore remains in each stage. These intervals are referred to as waiting times. In the quiescent stage, waiting times were very sensitive to the virus strain and presence of gangliosides (HA receptors) in the bilayer. When bilayers contained gangliosides, the waiting times in the Q stage for cells infected with the PR/8/34 strain of virus were exponentially distributed, whereas waiting times for cells infected with the Japan/305/57 strain were not so distributed. Without gangliosides, the waiting time distribution for PR/8/34 infected cells was complex. The waiting times in the R and S stages of pore growth were exponentially distributed under all tested conditions. Within the R stage, we analyzed the kinetics of the flickering pore by fitting the open and closed time distributions with a sum of two exponentials. Neither the open and closed time distributions nor the flickering pore conductance distributions were appreciably affected by virus strain or gangliosides. Colchicine and cytochalasin B increased the flicker rates, without affecting the waiting time in the R stage. We conclude that variations in amino acid sequences of the HAs and the presence of gangliosides as receptors within the target membrane critically affect the kinetics of fusion pore formation, but do not affect subsequent stages.     

Membrane permeability changes at early stages of influenza hemagglutinin-mediated fusion

While biological membrane fusion is classically defined as the leak-free merger of membranes and contents, leakage is a finding in both experimental and theoretical studies. The fusion stages, if any, that allow membrane permeation are uncharted. In this study we monitored membrane ionic permeability at early stages of fusion mediated by the fusogenic protein influenza hemagglutinin (HA). HAb2 cells, expressing HA on their plasma membrane, fused with human red blood cells, cultured liver cells PLC/PRF/5, or planar phospholipid bilayer membranes. With a probability that depended upon the target membrane, an increase of the electrical conductance of the fusing membranes (leakage) by up to several nS was generally detected. This leakage was recorded at the initial stages of fusion, when fusion pores formed. This leakage usually accompanied the "flickering" stage of the early fusion pore development. As the pore widened, the leakage reduced; concomitantly, the lipid exchange between the fusing membranes accelerated. We conclude that during fusion pore formation, HA locally and temporarily increases the permeability of fusing membranes. Subsequent rearrangement in the fusion complex leads to the resealing of the leaky membranes and enlargement of the pore.     

The fusion kinetics of influenza hemagglutinin expressing cells to planar bilayer membranes is affected by HA density and host cell surface

Time-resolved admittance measurements were used to follow formation of individual fusion pores connecting influenza virus hemagglutinin (HA)- expressing cells to planar bilayer membranes. By measuring in-phase, out-of-phase, and dc components of currents, pore conductances were resolved with millisecond time resolution. Fusion pores developed in stages, from small pores flickering open and closed, to small successful pores that remained open until enlarging their lumens to sizes greater than those of viral nucleocapsids. The kinetics of fusion and the properties of fusion pores were studied as functions of density of the fusion protein HA. The consequences of treating cell surfaces with proteases that do not affect HA were also investigated. Fusion kinetics were described by waiting time distributions from triggering fusion, by lowering pH, to the moment of pore formation. The kinetics of pore formation became faster as the density of active HA was made greater or when cell surface proteins were extensively cleaved with proteases. In accord with this faster kinetics, the intervals between transient pore openings within the flickering stage were shorter for higher HA density and more extensive cell surface treatment. Whereas the kinetics of fusion depended on HA density, the lifetimes of open fusion pores were independent of HA density. However, the lifetimes of open pores were affected by the proteolytic treatment of the cells. Faster fusion kinetics correlated with shorter pore openings. We conclude that the density of fusion protein strongly affects the kinetics of fusion pore formation, but that once formed, pore evolution is not under control of fusion proteins but rather under the influence of mechanical forces, such as membrane bending and tension.     

Initial size and dynamics of viral fusion pores are a function of the fusion protein mediating membrane fusion

Background information. Protein‐mediated merger of biological membranes, membrane fusion, is an important process. To investigate the role of fusogenic proteins in the initial size and dynamics of the fusion pore (a narrow aqueous pathway, which widens to finalize membrane fusion), two different fusion proteins expressed in the same cell line were investigated: the major glycoprotein of baculovirus Autographa californica (GP64) and the HA (haemagglutinin) of influenza X31. Results. The host Sf9 cells expressing these viral proteins, irrespective of protein species, fused to human RBCs (red blood cells) upon acidification of the medium. A high‐time‐resolution electrophysiological study of fusion pore conductance revealed fundamental differences in (i) the initial pore conductance; pores created by HA were smaller than those created by GP64; (ii) the ability of pores to flicker; only HA‐mediated pores flickered; and (iii) the time required for pore formation; HA‐mediated pores took much longer to form after acidification. Conclusion. HA and GP64 have divergent electrophysiological phenotypes even when they fuse identical membranes, and fusion proteins play a crucial role in determining initial fusion pore characteristics. The structure of the initial fusion pore detected by electrical conductance measurements is sensitive to the nature of the fusion protein.     

Single-channel analysis of the conductance fluctuations induced in lipid bilayer membranes by complement proteins C5b-9

Summary Single-channel analysis of electrical fluctuations induced in planar bilayer membranes by the purified human complement proteins C5b6, C7, C8, and C9 have been analyzed. Reconstitution experiments with lipid bilayer membranes showed that the C5b-9 proteins formed pores only if all proteins were present at one side of the membrane. The complement pores had an average single-channel conductance of 3.1 nS at 0.15m KCl. The histogram of the complement pores suggested a substantial variation of the size of the single channel. The linear relationship between single-channel conductance at fixed ionic strength and the aqueous mobility of the ions in the bulk aqueous phase indicated that the ions move inside the complement pore in a manner similar to the way they move in the aqueous phase. The minimum diameter of the pores as judged from the conductance data is approximately 3 nm. The complement channels showed no apparent voltage control or regulation up to transmembrane potentials of 100 mV. At neutral pH the pore is three to four times more permeable for alkali ions than for chloride, which may be explained by the existence of fixed negatively charged groups in or near the pore. The significance of these observations to current molecular models of the membrane lesion formed by these cytolytic serum proteins is considered.     

Estimation of the pore size of the large-conductance mechanosensitive ion channel of Escherichia coli.

The open channel diameter of Escherichia coli recombinant large-conductance mechanosensitive ion channels (MscL) was estimated using the model of Hille (Hille, B. 1968. Pharmacological modifications of the sodium channels of frog nerve. J. Gen. Physiol. 51:199-219) that relates the pore size to conductance. Based on the MscL conductance of 3.8 nS, and assumed pore lengths, a channel diameter of 34 to 46 A was calculated. To estimate the pore size experimentally, the effect of large organic ions on the conductance of MscL was examined. Poly-L-lysines (PLLs) with a diameter of 37 A or larger significantly reduced channel conductance, whereas spermine (approximately 15 A), PLL19 (approximately 25 A) and 1,1'-bis-(3-(1'-methyl-(4,4'-bipyridinium)-1-yl)-propyl)-4,4'-b ipyridinium (approximately 30 A) had no effect. The smaller organic ions putrescine, cadaverine, spermine, and succinate all permeated the channel. We conclude that the open pore diameter of the MscL is approximately 40 A, indicating that the MscL has one of the largest channel pores yet described. This channel diameter is consistent with the proposed homohexameric model of the MscL.     

Kinetics of folding of Escherichia coli OmpA from narrow to large pore conformation in a planar bilayer

The outer membrane protein of Escherichia coli, OmpA, is currently alleged to adopt two native conformations: a major two-domain conformer in which 171 N-terminal residues form a narrow eight beta-barrel pore and 154 C-terminal residues are in the periplasm and a minor one-domain conformer in which all 325 residues create a large pore. However, recent studies in planar bilayers indicate the conformation of OmpA is temperature-sensitive and that increasing temperature converts narrow pores to large pores. Here we examine the reversibility and kinetics of this transition for single OmpA molecules in planar bilayers of diphytanoylphosphatidylcholine (DPhPC). We find that the transition is irreversible. When temperatures are decreased, large pores close down, and when temperatures are stabilized they reopen in the large pore conformation, with gradually increasing open time. Large pores are converted to narrow pores only by denaturing agents. The transition from narrow to large pores requires temperatures >or= 26 degrees C and is a biphasic process with rates that rise steeply with temperature. The first phase, a flickering stepwise transition from a low-conductance to a high-conductance state requires approximately 7 h at 26 degrees C but only approximately 13 min at 42 degrees C, signifying an activation energy of 139 +/- 12 kJ/mol. This is followed by a gradual increase in conductance and open probability, interpreted as optimization of the large pore structure. The results indicate that the two-domain structure is a partially folded intermediate that is kinetically stable at lower temperatures and that mature fully folded OmpA is a large pore.     

Effects of Spontaneous Bilayer Curvature on Influenza Virus–mediated Fusion Pores

Cells expressing the hemagglutinin protein of influenza virus were fused to planar bilayer membranes containing the fluorescent lipid probes octadecylrhodamine (R18) or indocarbocyanine (DiI) to investigate whether spontaneous curvature of each monolayer of a target membrane affects the growth of fusion pores. R18 and DiI lowered the transition temperatures for formation of an inverted hexagonal phase, indicating that these probes facilitate the formation of negative curvature structures. The probes are known to translocate from one monolayer of a bilayer membrane to the other in a voltage-dependent manner. The spontaneous curvature of the cis monolayer (facing the cells) or the trans monolayer could therefore be made more negative through control of the polarity of voltage across the planar membrane. Electrical admittance measurements showed that the open times of flickering fusion pores were shorter when probes were in trans monolayers and longer when in cis monolayers compared with times when probe was symmetrically distributed. Open times were the same for probe symmetrically distributed as when probes were not present. Thus, open times were a function of the asymmetry of the spontaneous curvature between the trans and cis monolayers. Enriching the cis monolayer with a negative curvature probe reduced the probability that a small pore would fully enlarge, whereas enriching the trans monolayer promoted enlargement. Lysophosphatidylcholine has positive spontaneous curvature and does not translocate. When lysophosphatidylcholine was placed in trans leaflets of planar membranes, closing of fusion pores was rare. The effects of the negative and positive spontaneous curvature probes do not support the hypothesis that a flickering pore closes from an open state within a hemifusion diaphragm (essentially a “flat” structure). Rather, such effects support the hypothesis that the membrane surrounding the open pore forms a three-dimensional hourglass shape from which the pore flickers shut.     

Hemifusion between cells expressing hemagglutinin of influenza virus and planar membranes can precede the formation of fusion pores that subsequently fully enlarge

The chronological relation between the establishment of lipid continuity and fusion pore formation has been investigated for fusion of cells expressing hemagglutinin (HA) of influenza virus to planar bilayer membranes. Self-quenching concentrations of lipid dye were placed in the planar membrane to monitor lipid mixing, and time-resolved admittance measurements were used to measure fusion pores. For rhodamine-PE, fusion pores always occurred before a detectable amount of dye moved into an HA-expressing cell. However, with DiI in the planar membrane, the relationship was reversed: the spread of dye preceded formation of small pores. In other words, by using DiI as probe, hemifusion was clearly observed to occur before pore formation. For hemifused cells, a small pore could form and subsequently fully enlarge. In contrast, for cells that express a glycosylphosphatidylinositol-anchored ectodomain of HA, hemifusion occurred, but no fully enlarged pores were observed. Therefore, the transmembrane domain of HA is required for the formation of fully enlarging pores. Thus, with the planar bilayer membranes as target, hemifusion can precede pore formation, and the occurrence of lipid dye spread does not preclude formation of pores that can enlarge fully.     

Study of conductance changes of bilayer lipid membrane induced by electric field

Changes in the bilayer lipid membrane (BLM) conductance induced by electric field were studied. BLMs were formed from diphytanoylphosphocholine (DPhPC) solution in squalene. Certain time after a constant voltage (200-500 mV) was applied to the BLM in the voltage-clamp mode, the BLM conductance started to grow up to approximately 10 nS until the BLM ruptured. The conductance often changed abruptly (with the front duration of less than 33 micros) and then stabilized for a relatively long time (up to 10; 300 ms on average) thus resembling the ion channel activity. The mean amplitude of conductance steps was 650 pS. However, in some cases a slow conductance drift was recorded. When N-methyl-D-glucamine/glutamate ions were used instead of KCl, the conductance changes became 5 times smaller. We suggest that formation in the BLM of single pores approximately 1 nm in diameter should result in the observed changes in BLM conductance. The BLM conductance growth was due to consecutive opening of several such pores. When the electric field amplitude was abruptly decreased (down to 50-100 mV), the conductance dropped rapidly to the background value. When we increased the voltage again, the BLM conductance right after the increase depended on the time BLM spent under "weak" electric field. If this time exceeded 500 ms, the conductance was at the background level, but when the time was diminished, the conductance reached the value recorded before the voltage decrease. These data imply that the closure of the pores should lead to the formation in BLM of small defects (prepores) that can be easily transformed into pores when the voltage is increased. The lifetimes of such prepores did not exceed 500 ms.     

Inner but Not Outer Membrane Leaflets Control the Transition from Glycosylphosphatidylinositol-anchored Influenza Hemagglutinin-induced Hemifusion to Full Fusion

Cells that express wild-type influenza hemagglutinin (HA) fully fuse to RBCs, while cells that express the HA-ectodomain anchored to membranes by glycosylphosphatidylinositol, rather than by a transmembrane domain, only hemifuse to RBCs. Amphipaths were inserted into inner and outer membrane leaflets to determine the contribution of each leaflet in the transition from hemifusion to fusion. When inserted into outer leaflets, amphipaths did not promote the transition, independent of whether the agent induces monolayers to bend outward (conferring positive spontaneous monolayer curvature) or inward (negative curvature). In contrast, when incorporated into inner leaflets, positive curvature agents led to full fusion. This suggests that fusion is completed when a lipidic fusion pore with net positive curvature is formed by the inner leaflets that compose a hemifusion diaphragm. Suboptimal fusion conditions were established for RBCs bound to cells expressing wild-type HA so that lipid but not aqueous dye spread was observed. While this is the same pattern of dye spread as in stable hemifusion, for this “stunted” fusion, lower concentrations of amphipaths in inner leaflets were required to promote transfer of aqueous dyes. Also, these amphipaths induced larger pores for stunted fusion than they generated within a stable hemifusion diaphragm. Therefore, spontaneous curvature of inner leaflets can affect formation and enlargement of fusion pores induced by HA. We propose that after the HA-ectodomain induces hemifusion, the transmembrane domain causes pore formation by conferring positive spontaneous curvature to leaflets of the hemifusion diaphragm.     

Properties of the large ion-permeable pores formed from protein F of Pseudomonas aeruginosa in lipid bilayer membranes

The incorporation of porin protein F from the outer membrane of Pseudomonas aeruginosa into artificial lipid bilayers results in an increase of the membrane conductance by many orders of magnitude. The membrane conductance is caused by the formation of large ion-permeable channels with a single-channel conductance in the order of 5 nS for 1 M alkali chlorides. The conductance has an ohmic current vs. voltage relationship. Further information on the structure of the pore formed by protein F was obtained by determining the single-channel conductance for various species differing in charge and size, and from zero-current potential measurements. The channel was found to be permeable for large organic ions (Tris+, N(C2H5)4+, Hepes-) and a channel diameter of 2.2 nm could be estimated from the conductance data (pore length of 7.5 nm). At neutral pH the pore is about two times more permeable for cations than for anions, possibly caused by negative charges in the pore. The consistent observation of large water filled pores formed by porin protein F in model membrane systems is discussed in the light of the known low permeability of the Ps. aeruginosa outer membrane towards antibiotics. It is suggested that this results from a relatively low proportion of open functional porin protein F pores in vivo.