Two Distinct Modes of Exocytotic Fusion Pore Expansion in Large Astrocytic Vesicles

Formation of the fusion pore is a central question for regulated exocytosis by which secretory cells release neurotransmitters or hormones. Here, by dynamically monitoring exocytosis of large vesicles (2–7 μm) in astrocytes with two-photon microscopy imaging, we found that the exocytotic fusion pore was generated from the SNARE-dependent fusion at a ring shape of the docked plasma-vesicular membrane and the movement of a fusion-produced membrane fragment. We observed two modes of fragment movements, 1) a shift fragment that shifted to expand the fusion pore and 2) a fall-in fragment that fell into the collapsed vesicle to expand the fusion pore. Shift and fall-in modes are associated with full and partial collapses of large vesicles, respectively. The astrocytic marker, sulforhodamine 101, stained the fusion-produced membrane fragment more brightly than FM 1-43. Sulforhodamine 101 imaging showed that double fusion pores could simultaneously occur in a single vesicle (16% of large vesicles) to accelerate discharge of vesicular contents. Electron microscopy of large astrocytic vesicles showed shift and fall-in membrane fragments. Two modes of fusion pore formation demonstrate a novel mechanism underlying fusion pore expansion and provide a new explanation for full and partial collapses of large secretory vesicles.     

The dynamics of melittin-induced membrane permeability

The transport of co-encapsulated solutes through the melittin-induced pores in the membrane of giant phospholipid vesicles was studied, and the characteristics of the pore formation process were modeled. Molecules of two different sizes (dextran and the smaller, fluorescent marker Alexa Fluor) were encapsulated inside the vesicles. The chosen individual vesicles were then transferred by micromanipulation from the stock suspension to the environment with the melittin (MLT). The vesicles were observed optically with a phase-contrast microscope and by monitoring the fluorescence signal. Such an experimental setup enabled an analysis of a single vesicle’s response to the MLT on the basis of simultaneous, separate measurements of the outflow of both types of encapsulated molecules through the MLT-induced pores in the membrane. The mechanisms of the MLT’s action were suggested in a model for MLT pore formation, with oligomeric pores continuously assembling and dissociating in the membrane. Based on the model, the results of the experiments were explained as a consequence of the membrane’s permeability dynamics, with a continuously changing distribution of pores in the membrane with regard to their size and number. The relatively stable “average MLT pore” characteristics can be deduced from the proposed model.     

Indirect evidence of submicroscopic pores in giant unilamellar [correction of unilamelar] vesicles

Formation of pore-like structures in cell membranes could participate in exchange of matter between cell compartments and modify the lipid distribution between the leaflets of a bilayer. We present experiments on two model systems in which major lipid redistribution is attributed to few submicroscopic transient pores. The first kind of experiments consists in destabilizing the membrane of a giant unilamellar vesicle by inserting conic-shaped fluorescent lipids from the outer medium. The inserted lipids (10% of the vesicle lipids) should lead to membrane rupture if segregated on the outer leaflet. We show that a 5-nm diameter pore is sufficient to ease the stress on the membrane by redistributing the lipids. The second kind of experiments consists in forcing giant vesicles containing functionalized lipids to adhere. This adhesion leads to hemifusion (merging of the outer leaflets). In certain cases, the formation of pores in one of the vesicles is attested by contrast loss on this vesicle and redistribution of fluorescent labels between the leaflets. The kinetics of these phenomena is compatible with transient submicroscopic pores and long-lived membrane defects.     

Identification and characterization of the pore-forming protein in the outer membrane of rat liver mitochondria

The proteins of the outer membrane from rat liver mitochondria have been subfractionated by means of density gradient centrifugation. The different polypeptides of the membrane were incorporated into asolectin vesicles and black lipid membranes. It was observed that a polypeptide of M_r 32 000 renders asolectin vesicles permeable to ADP and forms pores in bilayer membrane. These pores showed the same properties as the channels which are formed in the lipid membrane after addition of Triton X-100 solubilized complete outer membrane. The properties of the pore are as follows: (1) The formation of pores depends on the type of phospholipid used for the preparation of the black membranes. (2) The pore is inserted asymmetrically into the membrane. (3) The pore is voltage gated but does not switch off completely at higher voltages. The pore seems to show different conductance states decreasing conductance being observed at increasing voltage. The implications of these findings for the regulation of transport processes across the outer membrane are discussed.     

Cascades of transient pores in giant vesicles: line tension and transport

Under ordinary circumstances, the membrane tension of a giant unilamellar vesicle is essentially nil. Using visible light, we stretch the vesicles, increasing the membrane tension until the membrane responds by the sudden opening of a large pore (several micrometers in size). Only a single pore is observed at a time in a given vesicle. However, a cascade of transient pores appear, up to 30-40 in succession, in the same vesicle. These pores are transient: they reseal within a few seconds as the inner liquid leaks out. The membrane tension, which is the driving force for pore opening, is relaxed with the opening of a pore and the leakage of the inner liquid; the line tension of the pore's edge is then able to drive the closure of a pore. We use fluorescent membrane probes and real-time videomicroscopy to study the dynamics of the pores. These can be visualized only if the vesicles are prepared in a viscous solution to slow down the leakout of the internal liquid. From measurements of the closure velocity of the pores, we are able to infer the line tension,. We have studied the effect of the shape of inclusion molecules on. Cholesterol, which can be modeled as an inverted cone-shaped molecule, increases the line tension when incorporated into the bilayers. Conversely, addition of cone-shaped detergents reduces. The effect of some detergents can be dramatic, reducing by two orders of magnitude, and increasing pore lifetimes up to several minutes. We give some examples of transport through transient pores and present a rough measurement of the leakout velocity of the inner liquid through a pore. We discuss how our results can be extended to less viscous aqueous solutions which are more relevant for biological systems and biotechnological applications.     

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.     

Fusion of phospholipid vesicles with planar phospholipid bilayer membranes. I. Discharge of vesicular contents across the planar membrane

Multilamellar phospholipid vesicles are introduced into the cis compartment on one side of a planar phospholipid bilayer membrane. The vesicles contain a water-soluble fluorescent dye trapped in the aqueous phases between the lamellae. If a vesicle containing n lamellae fuses with a planar membrane, an n-1 lamellar vesicle should be discharged into the opposite trans compartment, where it would appear as a discernible fluorescent particle. Thus, fusion events can be assayed by counting the number of fluorescent particles appearing in the trans compartment. In the absence of divalent cation, fusion does not occur, even after vesicles have been in the cis compartment for 40 min. When CaCl2 is introduced into the cis compartment to a concentration of greater than or equal to 20 mM, fusion occurs within the next 20 min; it generally ceases thereafter because of vesicle aggregation in the cis compartment. With approximately 3 x 10(8) vesicles/cm3 in the cis compartment, about 25-50 fusion events occur following CaCl2 addition. The discharge of vesicular contents across the planar membrane is the most convincing evidence of vesicle-membrane fusion and serves as a model for that ubiquitous biological phenomenon--exocytosis.     

Self-electroporation as a model for fusion pore formation

The creation of a small opening called the fusion pore is a necessary prerequisite for neurotransmitter release from synaptic vesicles. It is known that high intensity electric fields can create pores in vesicles by a process called electroporation. Due to the presence of charged phosphatidylserine (PS) molecules on the inner leaflet of the cell membrane, an electric field that is strong enough to cause electroporation of a synaptic vesicle might be present. It was shown by K. Rosenheck [K. Rosenheck. Biophys J 75, 1237-1243 (1998)] that in a planar geometry, fields sufficient to cause electroporation can occur at intermembrane separations of less than approximately 3 nm. It is frequently found, however, that the cell membrane is not planar but caves inward at the locations where a vesicle is close to it. Indentation of the cell membrane in the fusion region was modelled as a hemisphere and a theoretical study of the electric field in the vicinity of the cell membrane taking into account the screening effect of dissolved ions in the cytoplasm was performed. It was discovered that fields crossing the electroporation threshold occurred at a distance of 2 nm or less, supporting the claim that electroporation could be a possible mechanism for fusion pore formation.     

Ion leakage through transient water pores in protein-free lipid membranes driven by transmembrane ionic charge imbalance

We have employed atomic-scale molecular dynamics simulations to address ion leakage through transient water pores in protein-free phospholipid membranes. Our results for phospholipid membranes in aqueous solution with NaCl and KCl salts show that the formation of transient water pores and the consequent ion leakage can be induced and be driven by a transmembrane ionic charge imbalance, an inherent feature in living cells. These processes take place if the gradient is large enough to develop a sufficiently significant potential difference across the membrane. The transport of cations and anions through the water pores is then seen; it discharges the transmembrane potential, considerably reduces the size of a water pore, and makes the water pore metastable, leading eventually to its sealing. The ion transport is found to be sensitive to the type of ions. It turns out that Na(+) and Cl(-) ions leak through a membrane at approximately the same ratio despite the fact that Na(+) ions are expected to experience a lower potential barrier for the permeation through the pore. This is because of strong interactions of sodium ions with the carbonyl region of a phospholipid membrane as well as with lipid headgroups forming pore "walls," considerably slowing down the permeation of sodium ions. In contrast, we observed a pronounced selectivity of a phospholipid membrane to the permeation of potassium ions as compared to chloride ions: Potassium ions, being larger than sodium ions, interact only weakly with phospholipid headgroups, so that these interactions are not able to compensate for a large difference in free-energy barriers for permeation of K(+) and Cl(-) ions. These findings are found to be robust to a choice of force-field parameters for ions (tested by Gromacs and Charmm force-fields for ions). What is more, a potassium ion is found to be able to permeate a membrane along an alternate, "water-defect-mediated" pathway without actual formation of a pore. The "water-defect-mediated" leakage involves formation of a single water defect only and is found to be at least one order of magnitude faster than the pore-mediated ion leakage.     

Influence of proteins on the reorganization of phospholipid bilayers into large domains.

Using large (5-10 microns) vesicles formed in the presence of phospholipids fluorescently labeled on the acyl chain and visualized using a fluorescence microscope, charge-coupled-device camera, and digital image processor, we examined the effects of membrane proteins on phospholipid domain formation. In vesicles composed of phosphatidic acid and phosphatidylcholine, incubation with cytochrome c induced the reorganization of phospholipids into large phosphatidic acid-enriched domains with the exclusion of phosphatidylcholine. Cytochrome c binding was demonstrated to be highest in the phosphatidic acid-enriched domain of the vesicle using the absorbance of the heme moiety for visualization. Both binding of cytochrome c and phospholipid reorganization were blocked by pretreatment of the vesicles with 0.1 M NaCl. The pore forming peptide gramicidin was examined for the effects of an integral protein on domain formation. Initially, gramicidin distributed randomly within the vesicle and showed no phospholipid specificity. Phosphatidic acid domain formation in the presence of 2.0 mM CaCl2 or 100 microM cytochrome c was not affected by the presence of 5 mol % gramicidin within the vesicles. In both cases, gramicidin was preferentially excluded from the phosphatidic acid-enriched domain and became associated with phosphatidylcholine-enriched areas of the vesicle. Thus, cytochrome c caused a major reorganization of both the phospholipids and the proteins in the bilayer.     

Interaction of wheat alpha-thionin with large unilamellar vesicles.

The interaction of the wheat antibacterial peptide alpha-thionin with large unilamellar vesicles has been investigated by means of fluorescence spectroscopy. Binding of the peptide to the vesicles is followed by the release of vesicle contents, vesicle aggregation, and lipid mixing. Vesicle fusion, i.e., mixing of the aqueous contents, was not observed. Peptide binding is governed by electrostatic interactions and shows no cooperativity. The amphipatic nature of wheat alpha-thionin seems to destabilize the membrane bilayer and trigger the aggregation of the vesicles and lipid mixing. The presence of distearoylphosphatidylethanolamine-poly(ethylene glycol 2000) (PEG-PE) within the membrane provides a steric barrier that inhibits vesicle aggregation and lipid mixing but does not prevent leakage. Vesicle leakage through discrete membrane channels is unlikely, because the release of encapsulated large fluorescent dextrans is very similar to that of 8-aminonaphthalene-1,3,6,trisulfonic acid (ANTS). A minimum number of 700 peptide molecules must bind to each vesicle to produce complete leakage, which suggests a mechanism in which the overall destabilization of the membrane is due to the formation of transient pores rather than discrete channels.     

Mechanistic insights into the translocation of full length HIV-1 Tat across lipid membranes

The mechanism of how full length Tat (aa 1-86) crosses artificial lipid membranes was elucidated by means of fluorescence spectroscopy and fluorescence microscopy. It was shown that full length Tat (aa 1-86) neither forms pores in large unilamellar vesicles (LUVs) nor in giant unilamellar vesicles (GUVs) composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC). In contrast, an N-terminally truncated Tat protein (aa 35-86) that lacks the structurally defined proline- and cysteine-rich region as well as the highly conserved tryptophan residue at position 11 generates pores in artificial POPC-membranes, through which a water-soluble dye up to a size of 10kDa can pass. By means of fluorescence microscopy, the transfer of fluorescently labeled full length Tat across POPC-bilayers was unambiguously visualized with a concomitant accumulation of the protein in the membrane interface. However, if the dye was attached to the protein, also pore formation was induced. The size of the pores was, however smaller than the protein size, i.e. the labeled protein with a mass of 11.6kDa passed the membrane, while a fluorescent dye with a mass of 10kDa was excluded from the vesicles' interior. The results demonstrate that pore formation is not the prime mechanism by which full length Tat crosses a membrane.     

Ca++-induced fusion of fragmented sarcoplasmic reticulum with artificial planar bilayers

Summary Addition of fragmented sarcoplasmic reticulum (SR) vesicles to the aqueous phase of a black lipid membrane (BLM) causes a large increase in BLM conductance within 10 min. The conductance increase is absolutely dependent on three conditions: The presence of at least 0.5mm Ca⁺⁺, an acidic phospholipid such as phosphatidylserine or diphosphatidylglycerol in the BLM phospholipid mixture, and an osmotic gradient across the SR vesicle membrane, with the internal osmolarity greater than the external. These requirements are identical to conditions under which the fusion of phospholipid vesicles occurs.When the early part of the time course of conductance rise is examined at high sensitivity, the conductance is seen to increase in discrete steps. The probability of a step increases with the concentration of Ca⁺⁺ in the medium, with the fraction of acidic phospholipid in the BLM, and with the size of the osmotic gradient across the SR vesicle membrane. On the other hand, the average conductance change per step is independent of the above parameters, but varies with the type and concentration of ions present in the aqueous phase. For a given ion, the mean specific conductance per step is independent of the ion's concentration between 10 and 100mm.The probability distribution of the step-conductances agrees well with the distribution of SR vesicle surface areas, both before and after sonication of the vesicles.The evidence indicates that SR vesicles fuse with the BLM, thereby inserting SR membrane conductance pathways into it. Each discrete conductance jump appears to be the result of the fusion of a single SR vesicle with the BLM. This technique may serve as a general method for inserting membrane vesicles into an electrically accessible system.     

Ultradeformable lipid vesicles can penetrate the skin and other semi-permeable barriers unfragmented. Evidence from double label CLSM experiments and direct size measurements

The stability of various aggregates in the form of lipid bilayer vesicles was tested by three different methods before and after crossing different semi-permeable barriers. First, polymer membranes with pores significantly smaller than the average aggregate diameter were used as the skin barrier model; dynamic light scattering was employed to monitor vesicle size changes after barrier passage for several lipid mixtures with different bilayer elasticities. This revealed that vesicles must adapt their size and/or shape, dependent on bilayer stability and elasto-mechanics, to overcome an otherwise confining pore. For the mixed lipid aggregates with highly flexible bilayers (Transfersomes®), the change is transient and only involves vesicle shape and volume adaptation. The constancy of ultradeformable vesicle size before and after pores penetration proves this. This is remarkable in light of the very strong aggregate deformation during an enforced barrier passage. Simple phosphatidylcholine vesicles, with less flexible bilayers, lack such capability and stability. Conventional liposomes are therefore fractured during transport through a semi-permeable barrier; as reported by other researchers, liposomes are fragmented to the size of a narrow pore if sufficient pressure is applied across the barrier; otherwise, liposomes clog the pores. The precise outcome depends on trans-barrier flux and/or on relative vesicle vs. pore size. Lipid vesicles applied on the skin behave accordingly. Mixed lipid vesicles penetrate the skin if they are sufficiently deformable. If this is the case, they cross inter-cellular constrictions in the organ without significant composition or size modification. To prove this, we labelled vesicles with two different fluorescent markers and applied the suspension on intact murine skin without occlusion. The confocal laser scanning microscopy (CLSM) of the skin then revealed a practically indistinguishable distribution of both labels in the stratum corneum, corroborating the first assumption. To confirm the second postulate, we compared vesicle size in the starting suspension and in the blood after non-invasive transcutaneous aggregate delivery. Size exclusion chromatograms of sera from the mice that received ultradeformable vesicles on the skin were undistinguishable from the results measured with the original vesicle suspension. Taken together, the results support our previous postulate that ultradeformable vesicles penetrate the skin intact, that is, without permanent disintegration.     

Dehydroergosterol structural organization in aqueous medium and in a model system of membranes.

The aggregation of delta 5,7,9(11),22-ergostatetraen-3 beta-ol (dehydroergosterol or DHE), a fluorescent analog of cholesterol, was studied by photophysical techniques. It was concluded that the aqueous dispersions of DHE consist of strongly fluorescent microcrystals, and no evidence for self-quenching in micellar-type aggregates was found. The organization of DHE in model systems of membranes (phospholipid vesicles) is strongly dependent on the vesicle type. In small unilamellar vesicles, no evidence for aggregation is obtained, and the fluorescence anisotropy is rationalized on the basis of a random distribution of fluorophores. On the contrary, in large unilamellar vesicles (LUVs), a steeper concentration depolarization was observed. To explain this, a model that takes into account transbilayer dimer formation was derived. This was further confirmed from observation of excitonic absorption bands of 22-(N-7-nitrobenz-2-oxa-1,3-diazol-4-yl-amino)-23,24-bisnor- 5-cholen-3 beta-ol (NBD-cholesterol) in LUV, which disappear upon sonication. It is concluded that, in agreement with recent works, sterol aggregation is a very efficient process in large vesicles (and probably in natural membranes), even at very low concentrations (approximately 5 mol%).     

Pore formation and translocation of melittin.

Melittin, a bee venom, is a basic amphiphilic peptide, which mainly acts on the lipid matrix of membranes, lysing various cells. To elucidate the molecular mechanism, we investigated its interactions with phospholipid vesicles. The peptide formed a pore with a short lifetime in the membrane, as revealed by the release of an anionic fluorescent dye, calcein, from the liposomes. Our new double-labeling method clarified that the pore size increased with the peptide-to-lipid ratio. Upon the disintegration of the pore, a fraction of the peptides translocated across the bilayer. The pore formation was coupled with the translocation, which was proved by three fluorescence experiments recently developed by our laboratory. A novel model for the melittin pore formation was discussed in comparison with other pore-forming peptides.     

The curvature and cholesterol content of phospholipid bilayers alter the transbilayer distribution of specific molecular species of phosphatidylethanolamine

The curvature, cholesterol content, and transbilayer distribution of phospholipids significantly influence the functional properties of cellular membranes, yet little is known of how these parameters interact. In this study, the transbilayer distribution of phosphatidylethanolamine (PE) is determined in vesicles with large (98 nm) and small (19 nm) radii of curvature and with different proportions of PE, phosphatidylcholine, and cholesterol. It was found that the mean diameters of both types of vesicles were not influenced by their lipid composition, and that the amino-reactive compound 2,4,6-trinitrobenzenesulphonic acid (TNBS) was unable to cross the bilayer of either type of vesicle. When large vesicles were treated with TNBS, approximately 40% of the total membrane PE was derivatized; in the small vesicles 55% reacted. These values are interpreted as representing the percentage of total membrane PE residing in the outer leaflet of the vesicle bilayer. The large vesicles likely contained approximately 20% of the total membrane lipid as internal membranes. Therefore, in both types of vesicles, PE as a phospholipid class was randomly distributed between the inner and outer leaflets of the bilayer. The proportion of total PE residing in the outer leaflet was unaffected by changes in either the cholesterol or PE content of the vesicles. However, the transbilayer distributions of individual molecular species of PE were not random, and were significantly influenced by radius of curvature, membrane cholesterol content, or both. For example, palmitate- and docosahexaenoate-containing species of PE were preferentially located in the outer leaflet of the bilayer. Membrane cholesterol content affected the transbilayer distributions of stearate-, oleate-, and linoleate-containing species. The transbilayer distributions of palmitate-, docosahexaenoate-, and stearate-containing species were significantly influenced by membrane curvature, but only in the presence of high levels of cholesterol. Thus, differences in membrane curvature and cholesterol content alter the array of PE molecules present on the surfaces of phospholipid bilayers. In cells and organelles, these differences could have profound effects on a number of critical membrane functions and processes.     

Calcium-induced fusion of sea urchin egg secretory vesicles with planar phospholipid bilayer membranes.

The fusion of sea urchin egg secretory vesicles to planar phospholipid bilayer membranes was studied by differential interference contrast (DIC) and fluorescent microscopy, in combination with electrical recordings of membrane conductance. A strong binding of vesicles to protein-free planar membranes was observed in the absence of calcium. Calcium-induced fusion of vesicles was detected using two independent assays: loss of the contents of individual vesicles visible by DIC microscopy: and vesicle content discharge across the planar membrane detected by an increase in the fluorescence of a dye. In both cases, no increase in the membrane conductance was observed unless vesicles were incubated with either Amphotericin B or digitonin prior to applying them to the planar membrane, an indication that native vesicles are devoid of open channels. Pre-incubation of vesicles with n-ethylmaleimide (NEM) abolished calcium-induced fusion. Fusion was also detected when vesicles were osmotically swollen to the point of lysis. In contrast, no fusion of vesicles to planar bilayers was seen when vesicles on plasma membrane (native cortices) were applied to a phospholipid membrane, despite good binding of vesicles to the planar membrane and fusion of vesicles to plasma membrane. It is suggested that cortical vesicles (CVs) have sufficient calcium-sensitive proteins for fusion to lipid membranes, but in native cortices granular fusion sites are oriented toward the plasma membrane. Removal of vesicles from the plasma membrane may allow fusion sites on vesicles access to new membranes.     

Effect of surface curvature on the rate of cholesterol transfer between lipid vesicles.

The effect of surface curvature on the spontaneous movement of cholesterol between membranes was investigated by measuring the rates of cholesterol transfer from donor vesicles of various sizes to a common acceptor vesicle. Donor vesicles of size in the range 40-240 nm were prepared by extruding multilamellar dispersions through polycarbonate filters of different pore sizes under pressure. The smallest donor vesicle and the acceptor vesicles were obtained by the normal sonication procedures. The rate of cholesterol transfer, as measured by the movement of [3H]cholesterol, decreases with increasing size of the donor vesicle in an almost linear fashion. The extrapolation of the results gave a half-time (t1/2) of 16-20 h of the desorption of cholesterol from a planar bilayer, and this can be considered as a reference value for most cellular membranes which are characterized by very low curvatures. Our earlier studies have shown that the t1/2 for cholesterol efflux is influenced by the presence of gangliosides and phosphatidylethanolamine, and the asymmetric distribution of these lipids in the plasma membrane could partially account for the large difference in the rates of cholesterol movement from the two sides of the plasma membrane. The small differences in rates arising from asymmetric distribution will be magnified by the longer t1/2 obtained here for membranes of low curvatures, so that the large difference in rates might be a coupled effect of lipid asymmetry and low curvature of the plasma membrane. This, in turn, may have a role in maintaining the large differences in cholesterol/phospholipid molar ratios observed between plasma membrane and intracellular membranes.     

Release of small transmitters through kiss-and-run fusion pores in rat pancreatic beta cells

Exocytosis of secretory vesicles begins with a fusion pore connecting the vesicle lumen to the extracellular space. This pore may then expand or it may close to recapture the vesicle intact. The contribution of the latter, termed kiss-and-run, to exocytosis of pancreatic beta cell large dense-core vesicles (LDCVs) is controversial. Examination of single vesicle fusion pores demonstrated that rat beta cell LDCVs can undergo exocytosis by rapid pore expansion, by the formation of stable pores, or via small transient kiss-and-run fusion pores. Elevation of cAMP shifted LDCV fusion pore openings to the transient mode. Under this condition, the small fusion pores were sufficient for release of ATP, stored within LDCVs together with insulin. Individual ATP release events occurred coincident with amperometric "stand alone feet" representing kiss-and-run. Therefore, the LDCV kiss-and-run fusion pores allow small transmitter release but likely retain the larger insulin peptide. This may represent a mechanism for selective intraislet signaling.