Fusion and phase separation monitored by lifetime changes of a fluorescent phospholipid probe

The sensitivity of the fluorescence lifetime of 1-palmitoyl-2-[[2-[4- (6-phenyl-trans-1,3,5-hexatrienyl)phenyl]ethyl]carbonyl]- 3-sn-phosphatidylcholine (DPHpPC) to its local concentration in lipid bilayers was used to monitor both lipid mixing and phase separation occurring during membrane vesicle fusion. Vesicles containing 2 mol % DPHpPC were mixed with a 10-fold excess of vesicles devoid of probe. Upon addition of a fusogen, mixing of bilayer lipids associated with fusion was followed as an increase in the fluorescence lifetime of DPHpPC. Ca2+-induced fusion of phosphatidylserine vesicles served to test the method and was shown to have an exponential half-time of 7 s. Phase separation (between the phosphatidylserine head groups of bulk lipid and the phosphatidylcholine head groups of the probe) was monitored by DPHpPC under the same conditions used to follow lipid mixing due to fusion. Phase separation was not significant until 10 min after Ca2+ addition and was completely reversible by disodium ethylenediaminetetraacetate addition. Vesicle aggregation induced by Ca2+ addition to mixed phosphatidylserine/phosphatidylcholine vesicles did not alter the DPHpPC lifetime, indicating that close association of vesicles did not promote intervesicular exchange of the probe. In addition, we have investigated the effects of CA2+ on the fluorescence properties of this probe and of the head-group-labeled fluorescent probes N-(4-nitro-2,1,3-benzoxadiazolyl)phosphatidylethanolamine and N-(lissamine Rhodamine B sulfonyl)dioleoyl-phosphatidylethanolamine, which are used in the fluorescence energy transfer assay of Struck et al.(ABSTRACT TRUNCATED AT 250 WORDS)     

Comparative electrophysiological study of reconstituted giant vesicle preparations of the rabbit skeletal muscle sarcoplasmic reticulum K+ channel

Sarcoplasmic reticulum (SR) membranes isolated from rabbit skeletal muscle were reconstituted into two types of giant vesicles: (1) Giant proteoliposomes prepared by freeze-thawing of a mixture of SR vesicles and sonicated phospholipid vesicles without the use of detergent. (2) Giant SR vesicles prepared by fusion of SR vesicles using poly(ethylene glycol) (PEG) as a fusogen and without the addition of exogenous lipid. These giant vesicles were patch-clamped and properties of the single voltage-dependent potassium channel in the excised patch were studied. Single-channel conductance in a symmetrical solution of 0.1 M KCl and 1 mM CaCl2 was 140.0 +/- 10 pS (n = 5) for freeze-thawed vesicles and 136.4 +/- 15 pS (n = 7) for PEG vesicles. Both types of vesicles exhibited a sub-conductance state having 55% of the fully open state conductance. The voltage-dependence of open-channel probability could be expressed in terms of thermodynamic parameters of delta Gi = 0.95 kcal/mol and z = -0.77 for freeze-thawed vesicles and delta Gi = 0.92 kcal/mol and z = -0.87 for PEG vesicles. These values correlated well with previous data obtained by fusion of native SR vesicles with a planar lipid membrane. Channel orientation was found to be conserved in both types of vesicles used in the present study.     

Effects of hemagglutinin fusion peptide on poly(ethylene glycol)-mediated fusion of phosphatidylcholine vesicles.

The effects of hemagglutinin (HA) fusion peptide (X-31) on poly(ethylene glycol)- (PEG-) mediated vesicle fusion in three different vesicle systems have been compared: dioleoylphosphatidylcholine (DOPC) small unilamellar vesicles (SUV) and large unilamellar vesicles (LUV) and palmitoyloleoylphosphatidylcholine (POPC) large unilamellar perturbed vesicles (pert. LUV). POPC LUVs were asymmetrically perturbed by hydrolyzing 2.5% of the outer leaflet lipid with phospholipase A(2) and removing hydrolysis products with BSA. The mixing of vesicle contents showed that these perturbed vesicles fused in the presence of PEG as did DOPC SUV, but unperturbed LUV did not. Fusion peptide had different effects on the fusion of these different types of vesicles: fusion was not induced in the absence of PEG or in unperturbed DOPC LUV even in the presence of PEG. Fusion was enhanced in DOPC SUV at low peptide surface occupancy but hindered at high surface occupancy. Finally, fusion was hindered in proportion to peptide concentration in perturbed POPC LUV. Contents leakage assays demonstrated that the peptide enhanced leakage in all vesicles. The peptide enhanced lipid transfer between both fusogenic and nonfusogenic vesicles. Peptide binding was detected in terms of enhanced tryptophan fluorescence or through transfer of tryptophan excited-state energy to membrane-bound diphenylhexatriene (DPH). The peptide had a higher affinity for vesicles with packing defects (SUV and perturbed LUV). Quasi-elastic light scattering (QELS) indicated that the peptide caused vesicles to aggregate. We conclude that binding of the fusion peptide to vesicle membranes has a significant effect on membrane properties but does not induce fusion. Indeed, the fusion peptide inhibited fusion of perturbed LUV. It can, however, enhance fusion between highly curved membranes that normally fuse when brought into close contact by PEG.     

Mechanism of the spontaneous transfer of unconjugated bilirubin between small unilamellar phosphatidylcholine vesicles.

Unconjugated bilirubin (bilirubin-IX alpha), the hydrophobic end product of heme degradation, is esterified in the hepatocyte endoplasmic reticulum to water-soluble conjugates prior to excretion in bile. To characterize the process of intracellular bilirubin transport, the kinetic and thermodynamic activation parameters for the spontaneous transfer of bilirubin between small unilamellar egg lecithin vesicles were determined. Bilirubin-IX alpha was added to donor vesicles labeled with the fluorescent phospholipid probe, (5-(dimethylamino)naphthalene-1-sulfonyl) dipalmitoyl-L-alpha-phosphatidylethanolamine (dansyl-PE). When bound to the donor vesicles, bilirubin quenches the dansyl probe fluorescence through resonance energy transfer. The movement of bilirubin from dansyl-labeled donor vesicles to unlabeled acceptor vesicles was monitored directly by the reemergence of dansyl fluorescence over time. Vesicle fusion and intervesicle transfer of the dansyl-PE probe were excluded by quasielastic light scattering and fluorescence resonance energy transfer studies. Stopped-flow analysis demonstrated that the transfer of bilirubin was described by a single-exponential function with a mean half-time of 2.0 +/- 0.1 ms (+/- SD) at 37 degrees C. The rate of bilirubin transfer was independent of acceptor vesicle concentration and decreased with increasing buffer ionic strength, indicating that intermembrane transfer occurred via aqueous diffusion, rather than vesicle collisions. The free energy of activation (delta G++) for the dissociation of bilirubin from donor vesicles was 14.2 kcal.mol-1. These studies suggest that bilirubin is associated with phospholipid bilayers at the membrane-water interface. We postulate that the movement of unconjugated bilirubin between intracellular membranes occurs via spontaneous transfer through the aqueous phase.     

The rate of lipid transfer during fusion depends on the structure of fluorescent lipid probes: a new chain-labeled lipid transfer probe pair.

A number of fluorescent probes have been used to follow membrane fusion events, particularly intermixing of lipids. None of them is ideal. The most popular pair of probes is NBD-PE and Rh-PE, in which the fluorescent groups are attached to the lipid headgroups, making them sensitive to changes in the surrounding medium. Here we present a new assay for monitoring lipid transfer during membrane fusion using the acyl chain tagged fluorescent probes BODIPY500-PC and BODIPY530-PE. Like the NBD-PE/Rh-PE assay, this assay is based on fluorescence resonance energy transfer (FRET) between the donor, BODIPY500, and the acceptor, BODIPY530. The magnitude of FRET is sensitive to the probe surface concentration, allowing one to detect movement of probes from labeled to unlabeled vesicles during fusion. The high quantum yield of fluorescence, high efficiency of FRET (R(o) is estimated to be approximately 60 A), photostability, and localization in the central hydrophobic region of a bilayer all make this pair of probes quite promising for detecting fusion. We have compared this and two other lipid mixing assays for their abilities to detect the initial events of poly(ethylene glycol) (PEG)-mediated fusion of small unilamellar vesicles (SUVs). We found that the BODIPY500/530 assay showed lipid transfer rates consistent with those obtained using the DPHpPC self-quenching assay, while lipid mixing rates measured with the NBD-PE/Rh-PE RET assay were significantly slower. We speculate that the bulky labeled headgroups of NBD-PE and especially Rh-PE molecules hamper movement of probes through the stalk between fusing vesicles, and thus reduce the apparent rate of lipid mixing.     

Bilayer curvature and certain amphipaths promote poly(ethylene glycol)-induced fusion of dipalmitoylphosphatidylcholine unilamellar vesicles.

Unilamellar vesicles of varying and reasonably uniform size were prepared from 1,2-dipalmitoyl-3-sn-phosphatidylcholine (DPPC) by the extrusion procedure and sonication. Quasi-elastic light scattering was used to show that different vesicle preparations had mean (Z-averaged) diameters of 1340, 900, 770, 630, and 358 A (sonicated). Bilayer-phase behavior as detected by differential scanning calorimetry was consistent with the existence of essentially uniform vesicle populations of different sizes. The response of these different vesicles to treatment with poly(ethylene glycol) (PEG) was monitored using fluorescence assays for lipid transfer, contents leakage, and contents mixing, as well as quasi-elastic light scattering. No fusion, as judged by vesicle contents mixing and change in vesicle size, was detected for vesicles of diameter greater than 770 A. The diameters of smaller vesicles increased dramatically when treated with high concentrations of PEG, although mixing of their contents could not be detected both because of their small trapped volumes and because of the extensive leakage induced in small vesicles by high concentrations of PEG. Lipid transfer was detected between vesicles of all sizes. We conclude the high bilayer curvature does encourage fusion of closely juxtaposed membrane bilayers but that highly curved vesicles appear also to rupture and form larger structures when diluted from high PEG concentration, a process that can be confused with fusion. Despite the failure of PEG to induce fusion of large, uncurved vesicles composed of a single phosphatidylcholine, these vesicles can be induced to fuse when they contain small amounts of certain amphiphathic compounds thought to play a role in cellular fusion processes. Thus, vesicles which contained 0.5 mol % L-alpha-lysopalmitoylphosphatidylcholine, 5 mol % platelet activating factor, or 0.5 mol % palmitic acid fused in the presence of 30%, 25%, and 20% (w/w) PEG, respectively. However, vesicles containing 1,2-dipalmitoyl-sn-glycerol, 1,2-dioleoyl-sn-glycerol, 1-oleoyl-2-acetyl-sn-glycerol, or monooleoyl-rac-glycerol at surface concentrations up to 5 mol % did not fuse in the presence or absence of PEG. There was no correlation between the abilities of these amphipaths to induce phase separation or nonlamellar phases and their abilities to support fusion of pure DPPC unilamellar vesicles in the presence of high concentrations of PEG. The results are discussed in terms of the type of disrupted lipid packing that could be expected to favor PEG-mediated fusion.     

Poly(ethylene glycol)-induced lipid mixing but not fusion between synthetic phosphatidylcholine large unilamellar vesicles

We have examined the effect of poly(ethylene glycol) (PEG) on stable large unilamellar vesicles formed by a rapid extrusion technique and composed of pure synthetic phosphatidylcholines. The lipid systems studied were the saturated 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) and the monounsaturated 1,2-dioleoyl-sn-glycerol-3-phosphocholine (DOPC). PEG at all concentrations (3.8-40 wt %) induced lipid mixing between large vesicles composed of these phosphatidylcholines. Extensive leakage of internal contents also occurred at high PEG concentrations. However, in contrast to our previous report [Parente, R. A., & Lentz, B. R. (1986) Biochemistry 25, 6678], we could detect no mixing of internal contents indicative of fusion. This discrepancy is due to environmental factors that affect the behavior of 8-amino-naphthalene-1,3,6-trisulfonic acid (ANTS), the fluorophore used in the assay for contents mixing and leakage [McIntyre, Parks, Massenburg, & Lentz (1991) (submitted)]. In agreement with the results of the fusion assay, quasielastic light-scattering measurements revealed no increase in vesicle size following treatment with PEG. These results emphasize the importance of using assays for both membrane mixing and contents mixing to demonstrate fusion, since significant lipid mixing occurred in the absence of fusion. We conclude that large vesicles composed of pure phosphatidylcholine do not fuse in the presence of even high concentrations of PEG. However, DOPC vesicles containing a small amount of an amphipathic "impurity" have been shown to fuse in the presence of PEG at 23 degrees C. These results are discussed in terms of their implications for the mechanism of PEG-induced membrane fusion.     

Fusion of lipid vesicles with ascites tumor cells and their lipid-depleted variants. Studies with radioactive- and fluorescent-labeled vesicles

Cultured ascites tumor cells and their lipid-depleted variants, which contained 35-40% less membrane phospholipid and cholesterol, were used for fusion experiments with unilamellar lipid vesicles which were between 300 and 600 nm in diameter. Vesicle-cell interaction was followed by tracer studies using vesicles double-labeled in the lipid moiety, by vesicle-encapsulated [3H] dextran, and by measurements of energy transfer between N-(10-[1-pyrene]decanoyl)sphingomyelin-labeled vesicles and alpha-parinaric acid-labeled cells in the presence of poly(ethylene glycol) (PEG) as fusogen. The reaction rates measured with the radiolabeled vesicles were found to follow patterns similar to those obtained with the resonance energy transfer assay. This latter method revealed a vesicle-cell membrane fusion reaction, which was substantiated by radiolabeling the internal cellular compartment after treatment of the cells with [3H]dextran-encapsulated vesicles as shown by electron microscopic autoradiography on semi-thin sections. Endocytosis as a reaction mechanism can be excluded, since no energy transfer was observed at 25 degrees C in the absence of PEG. Investigations of vesicle bilayer order and fluidity on vesicle-cell interaction revealed optimal reactivity, with intermediate fluidity corresponding to cholesterol/phospholipid ratios between 0.7 and 1.0 and fluorescence depolarization (P) values of 0.18 and 0.21. Lipid depletion decreased the reaction velocity between cells and vesicles by about 20%, exhibiting V values of 33.2 mumol/min, as compared to the control of 41.4 mumol/min determined for 10(7) cells. The affinity constants for vesicle lipid were affected only slightly with Km values of 0.195 mM (0.210 mM). The activation energies for the reaction were calculated to give values of EA = 22.44 kJ/mol for the control and of EA = 20.4 kJ/mol for the modified cells. These data indicate that the decrease in membrane lipid content apparently has no major influence on the extent of the interaction.     

Reduction of cytochrome b5 by NADPH-cytochrome P450 reductase

The reduction of mammalian cytochrome b5 (b5) by NADPH-cytochrome P450 (P450) reductase is involved in a number of biological reactions. The kinetics of the process have received limited consideration previously, and a combination of pre-steady-state (stopped-flow) and steady-state approaches was used to investigate the mechanism of b5 reduction. In the absence of detergent or lipid, a reductase-b5 complex is formed and rearranges slowly to an active form. Electron transfer to b5 is rapid within this complex (>30 s(-1) at 23 degrees C), as fast as to cytochrome c. With excess b5 present, a burst of reduction is observed, consistent with rapid electron transfer to one or two b5 molecules per reductase, followed by a subsequent rate-limiting event. In detergent vesicles, the reductase and b5 interact rapidly but electron transfer is slower (approximately 3 s(-1) at 23 degrees C). Experiments with dimyristyl lecithin vesicles yielded results intermediate between the non-vesicle and detergent systems. These steady-state and pre-steady-state kinetics provide views of the different natures of the reduction of b5 by the reductase in the absence and presence of vesicles. Without vesicles, the encounter of the reductase and b5 is rapid, followed by a slow reorganization of the initial complex (approximately 0.07 s(-1)), very fast reduction, and dissociation. In vesicles, encounter is rapid and the slow step (approximately 3 s(-1)) is reduction within a complex less favorable for reduction than in the non-vesicle systems.     

Influence of gp41 fusion peptide on the kinetics of poly(ethylene glycol)-mediated model membrane fusion

The fusion peptide of the HIV fusion protein gp41 is required for viral fusion and entry into a host cell, but it is unclear whether this 23-residue peptide can fuse model membranes. We address this question for model membrane vesicles in the presence and absence of aggregating concentrations of poly(ethylene glycol) (PEG). PEG had no effect on the physical properties of peptide bound to membranes or free in solution. We tested for fusion of both highly curved and uncurved PC/PE/SM/CH (35:30:15:20 mol %) vesicles and highly curved PC/PE/CH (1:1:1) vesicles treated with peptide in the presence and absence of PEG. Fusion was never observed in the absence of PEG, although high peptide concentrations led to aggregation and rupture, especially in unstable PC/PE/CH (1:1:1) vesicles. When 5 wt % PEG was present to aggregate vesicles, peptide enhanced the rate of lipid mixing between curved PC/PE/SM/CH vesicles in proportion to the peptide concentration, with this effect leveling off at peptide/lipid (P/L) ratios approximately 1:200. Peptide produced an even larger effect on the rate of contents mixing but inhibited contents mixing at P/L ratios >1:200. No fusion enhancement was seen with uncurved vesicles. The rate of fusion was also enhanced by the presence of hexadecane, and peptide-induced rate enhancement was not observed in the presence of hexadecane. We conclude that gp41 fusion peptide does not induce vesicle fusion at subrupturing concentrations but can enhance fusion between highly curved vesicles induced to fuse by PEG. The different effects of peptide on the rates of lipid mixing and fusion pore formation suggest that, while gp41 fusion peptide does affect hemifusion, it mainly affects pore formation.     

Kinetics of fluorescent-labeled phosphatidylcholine transfer between nonspecific lipid transfer protein and phospholipid vesicles

Recently, rat liver nonspecific lipid transfer protein (nsLTP) was shown to form a fluorescent complex when allowed to equilibrate with self-quenching vesicles prepared from the fluorescent phospholipid 1-palmitoyl-2-[12-[(7-nitro-2,1,3-benzoxadiazol-4- yl)amino]dodecanoyl]phosphatidylcholine (P-C12-NBD-PC) [Nichols, J. W. (1987) J. Biol. Chem. 262, 14172-14177]. Investigation of the mechanism of complex formation was continued by studying the kinetics of transfer of P-C12-NBD-PC between nsLTP and phospholipid vesicles using a transfer assay based on resonance energy transfer between P-C12-NBD-PC and N-(lissamine rhodamine B sulfonyl)dioleoylphosphatidylethanolamine. The principles of mass action kinetics (which predict initial lipid transfer rates as a function of protein and vesicle concentration) were used to derive equations for two distinct mechanisms: lipid transfer by the diffusion of monomers through the aqueous phase and lipid transfer during nsLTP-membrane collisions. The results of these kinetics studies indicated that the model for neither mechanism alone adequately predicted the initial rates of formation and dissolution of the P-C12-NBD-PC-nsLTP complex. The initial rate kinetics for both processes were predicted best by a model in which monomer diffusion and collision-dependent transfer occur simultaneously. These data support the hypothesis that the phospholipid-nsLTP complex functions as an intermediate in the transfer of phospholipids between membranes.     

Plasma cholesteryl ester transfer protein has binding sites for neutral lipids and phospholipids

The plasma cholesteryl ester-transfer protein (CETP, Mr 74,000) promotes exchange of both neutral lipids and phospholipids (phosphatidylcholine, PC) between lipoproteins. To investigate the mechanism of facilitated lipid transfer, CETP was incubated with unilamellar egg PC vesicles containing small amounts of cholesteryl ester (CE) or triglyceride, and then analyzed by gel filtration chromatography. There was rapid transfer of radiolabeled CE or triglyceride and PC from vesicles to CETP. The CETP with bound lipids was isolated and incubated with low density lipoproteins (LDL), resulting in transfer of the lipids to LDL. The CETP bound up to 0.9 mol of CE or 0.2 mol of triglyceride and 11 mol of PC/mol of CETP. para-Chloromercuriphenylsulfonate, an inhibitor of CE and triglyceride transfer, was found to decrease the binding of radiolabeled CE and triglyceride by CETP. Under various conditions the CETP eluted either as an apparent monomer with bound lipid (Mr 75,000-93,000), or in complexes with vesicles. The distribution of CETP between these two states was influenced by the presence of apoA-I or albumin, incubation time, vesicle/CETP ratio, and buffer pH and ionic strength. The results indicate that the CETP has binding sites for CE, triglyceride, and PC which readily equilibrate with lipoprotein lipids and suggest that CETP can act as a carrier of lipid between lipoproteins.     

Rate and extent of poly(ethylene glycol)-induced large vesicle fusion monitored by bilayer and internal contents mixing

Poly(ethylene glycol) (PEG) of average molecular weight 8000 was used to mediate the fusion of large unilamellar vesicles composed of dipalmitoylphosphatidylcholine. Fusion was monitored by fluorescence assays of lipid mixing and aqueous contents mixing. The extent of lipid mixing, as monitored by DPHpPC fluorescence lifetime, indicated that large unilamellar vesicles underwent a single fusion cycle when incubated with PEG and subsequently diluted into buffer. The ANTS/DPX assays for contents mixing and leakage indicated that, while addition and dilution of PEG were accompanied by extensive contents leakage, this occurred on a much different time scale as compared to contents mixing. Both the lipid-mixing and contents-mixing assays gave comparable estimates for the number of rounds of fusion that occurred in a given time following PEG addition, although the contents-mixing assay always yielded an estimate 10-15% larger than the lipid-mixing assay. These assays were used to evaluate several factors purported to influence PEG-induced fusion. First, the initial rate of fusion was found to be dependent on PEG concentration in the range of 0-35 wt %, while the extent of fusion was not. In addition, a substantial rate enhancement occurred when vesicles were incubated with greater than 26% PEG. Second, the creation of an osmotic gradient upon dilution of vesicle-PEG mixtures was shown to have no effect on either the extent or the initial rate of fusion. Consistent with this observation, both contents and lipid mixing were found to occur prior to and independent of the dilution of the PEG-vesicle suspension. Third, impurities, either present in our commercially available PEG or added to vesicle-PEG mixtures, also had no effect on the rate or extent of fusion. Fourth, another dehydrating polymer, dextran (average mol wt 9000), was capable of promoting fusion, though at a much lower rate than PEG. These results suggest that even partial bilayer dehydration accompanied by vesicle collapse and close interbilayer contact may be sufficient to induce vesicle fusion.     

Advantages and limitations of 1-palmitoyl-2-[[2-[4- (6-phenyl-trans-1,3,5-hexatrienyl)phenyl]ethyl]carbonyl]-3- sn-phosphatidylcholine as a fluorescent membrane probe

We have investigated the behavior of 1-palmitoyl-2-[[2-[4- (6-phenyl-trans-1,3,5-hexatrienyl)phenyl]ethyl]carbonyl]-3-sn -phosphatidylcholine (DPHpPC) in synthetic, multilamellar phosphatidylcholine vesicles. This fluorescent phospholipid has photophysical properties similar to its parent fluorophore, diphenylhexatriene (DPH). DPHpPC preferentially partitioned into fluid phase lipid (Kf/s = 3.3) and reported a lower phase transition temperature as detected by fluorescence anisotropy than that observed by differential scanning calorimetry. Calorimetric measurements of the bilayer phase transition in samples having different phospholipid to probe ratios demonstrated very slight changes in membrane phase transition temperature (0.1-0.2 degree C) and showed no measurable change in transition width. Nonetheless, measurements of probe fluorescence properties suggested that DPHpPC disrupts its local environment in the membrane and may even induce perturbed probe-rich local domains below the phospholipid phase transition. Temperature profiles of steady-state fluorescence anisotropy, limiting anisotropy, differential tangent, and rotational rate were similar to those of DPH below the main lipid phase transition but indicated more restricted rotational motion above the lipid phase transition temperature. As for DPH, the fluorescence decay of DPHpPC could be described by either a single or double exponential both above and below the DPPC phase transition. The choice seemed dependent on the treatment of the sample. The intensity-weighted average lifetime of DPHpPC was roughly 1.5 ns shorter than that of DPH. In summary, the measured properties of DPHpPC and its lipid-like structure make it a powerful probe of membrane structure and dynamics.     

Human platelet factor 4 subunit association/dissociation thermodynamics and kinetics

Platelet factor 4 (PF4) monomers (7800 daltons) form dimers and tetramers in varying molar ratios under certain solution conditions [Mayo, K. H., & Chen, M. J. (1989) Biochemistry 28, 9469]. The presence of a simplified aromatic region (one Tyr and two His) and resolved monomer, dimer, and tetramer Y60 3,5 ring proton resonances makes study of PF4 aggregate association/dissociation thermodynamics and kinetics possible. PF4 protein subunit association/dissociation equilibrium thermodynamic parameters have been derived by 1H NMR (500MHz) resonance line-fitting analysis of steady-state Y60 3,5 ring proton resonance monomer-dimer-tetramer populations as a function of temperature from 10 to 40 degrees C. Below 10 degrees C and above 40 degrees C, resonance broadening and overlap severely impaired analysis. Enthalpic and entropic contributions to dimer association Gibb's free energy [-5.1 kcal/mol (30 degrees C)] are +2.5 +/- 1 kcal/mol and +26 +/- 7 eu, respectively, and for tetramer association Gibb's free energy [-5.7 kcal/mol (30 degrees C)], they are -7.5 +/- 1 kcal/mol and -7 +/- 3 eu, respectively. These thermodynamic parameters are consistent with low dielectric medium electrostatic/hydrophobic interactions governing dimer formation and hydrogen bonding governing tetramer formation. Association/dissociation kinetic parameters, i.e., steady-state jump rates, have been derived from exchange-induced line-width increases and from 1H NMR (500 MHz) saturation-transfer and spin-lattice (Tl) relaxation experiments. From dissociation jump rates and equilibrium constants, association rate constants were estimated. For dimer and tetramer equilibria at 30 degrees C, unimolecular dissociation rate constants are 35 +/- 10 s-1 for dimer dissociation and 6 +/- 2 s-1 for tetramer dissociation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Interaction of intestinal brush border membrane vesicles with small unilamellar phospholipid vesicles. Exchange of lipids between membranes is mediated by collisional contact

The kinetics of lipid transfer from small unilamellar vesicles as the donor to brush border vesicles as the acceptor have been investigated by following the transfer of radiolabeled or spin-labeled lipid molecules in the absence of exchange protein. The labeled lipid molecules studied were various radiolabeled and spin-labeled phosphatidylcholines, radiolabeled cholesteryl oleate, and a spin-labeled cholestane. At a given temperature and brush border vesicle concentration similar pseudo-first-order rate constants (half-lifetimes) were observed for different lipid labels used. The lipid transfer is shown to be an exchange reaction leading to an equal distribution of label in donor and acceptor vesicles at equilibrium (time t----infinity). The lipid exchange is a second-order reaction with rate constants being directly proportional to the brush border vesicle concentration. The results are only consistent with a collision-induced exchange of lipid molecules between small unilamellar phospholipid vesicles and brush border vesicles. Other mechanisms such as collision-induced fusion or diffusion of lipid monomers through the aqueous phase are negligible at least under our experimental conditions.     

Thermodynamics of the binding of human apolipoprotein A-I to dimyristoylphosphatidylglycerol

The interaction of human serum apolipoprotein A-I with dimyristoylphosphatidylglycerol was analyzed by isothermal titration calorimetry. Binding of the apolipoprotein A-I to large unilamellar vesicles of dimyristoylphosphatidylglycerol, a negatively charged phospholipid, is characterized by thermodynamic parameters which are invariant over the 30-40 degrees C temperature range. The enthalpy change resulting from the first additions of lipid are positive and decline in magnitude with subsequent additions of lipid. After several additions of lipid, the sign of the enthalpy changes to negative and then reaches a constant value/injection. This exothermic process is larger and opposite in sign to the heat of dilution. Similar behavior is also observed when the lipid is in the form of a dispersion in distilled water. Only a non-saturable exothermic process is observed at 30 degrees C with large unilamellar vesicles of the zwitterionic lipid, dimyristoylphosphatidylcholine. The beginning of an exothermic process can also be observed prior to the larger endotherm in the first injections of large unilamellar vesicles of dimyristoylphosphatidylglycerol into the protein. We analyze the enthalpy changes for the reaction of dimyristoylphosphatidylglycerol with the protein as arising from two distinct processes, one endothermic and the other exothermic. The binding isotherms for the high affinity binding of the apolipoprotein A-I to large unilammelar vesicles of dimyristoylphosphatidylglycerol, over the temperature range 30-40 degrees C, gave an enthalpy change of 1.43 +/- 0.07 kcal/mol of protein and a free energy change of -5.91 +/- 0.04 kcal/mol of protein for the binding of the protein to a cluster of 25 +/- 2 lipid molecules. Thus this reaction is entropically driven.     

Direct simulation of protein-mediated vesicle fusion: lung surfactant protein B

We simulated spontaneous fusion of small unilamellar vesicles mediated by lung surfactant protein B (SP-B) using the MARTINI force field. An SP-B monomer triggers fusion events by anchoring two vesicles and facilitating the formation of a lipid bridge between the proximal leaflets. Once a lipid bridge is formed, fusion proceeds via a previously described stalk - hemifusion diaphragm - pore-opening pathway. In the absence of protein, fusion of vesicles was not observed in either unbiased simulations or upon application of a restraining potential to maintain the vesicles in close proximity. The shape of SP-B appears to enable it to bind to two vesicles at once, forcing their proximity, and to facilitate the initial transfer of lipids to form a high-energy hemifusion intermediate. Our results may provide insight into more general mechanisms of protein-mediated membrane fusion, and a possible role of SP-B in the secretory pathway and transfer of lung surfactant to the gas exchange interface.     

Mechanism of vitamin A movement between rod outer segments, interphotoreceptor retinoid-binding protein, and liposomes

Vitamin A movement between rod outer segment (ROS) membranes, interphotoreceptor retinoid-binding protein (IRBP), and liposomes was examined by two different methods. Equilibrium exchange of all-trans-retinol was followed by assessing the transfer of [3H]retinol from liposomes to ROS membranes as compared to a nontransferable marker, [14C]triolein. In the absence of IRBP, a rapid, spontaneous transfer of [3H] retinol to the ROS membranes occurred. In the presence of 2 microM IRBP, retinol transfer decreased by approximately one-half, whereas a similar concentration of bovine serum albumin had no effect on this spontaneous transfer. Kinetics of retinol transfer between single unilamellar vesicles were determined by the method of fluorescence energy transfer. The first order rate constant for this transfer was 0.85 s-1 at 22 degrees C at either pH 7.4 or pH 2.8. This rate was not affected by varying the concentration of acceptor vesicles 50-fold or by varying their concentration 10-fold at a constant ratio of donor-to-acceptor vesicles. The presence of IRBP as an additional acceptor did not change the rate. The transfer was temperature-dependent with an activation energy of 7.8 kcal/mol. The transfer rate appeared to be an increasing exponential function of ionic strength since high concentrations of NaCl decreased the transfer rate significantly. The transfer rate of retinol from IRBP to single unilamellar vesicles also followed first order kinetics with a rate constant of 0.11 s-1 at 22 degrees C, which was approximately 8 times slower than that of transfer between vesicles. We conclude that the transfer of all-trans-retinol between liposomes and membranes can be accomplished rapidly via the aqueous phase, and that IRBP retards rather than facilitates this transfer process.     

Phospholipid transfer between phosphatidylcholine-taurocholate mixed micelles

The transfer of fluorescent-labeled N-(7-nitro-2,1,3-benzoxadiazol-4-yl)phosphatidylethanolamine (N-NBD-PE) between phosphatidylcholine-taurocholate mixed micelles was measured by monitoring the increase in fluorescence as N-NBD-PE, initially contained in mixed micelles at self-quenching concentrations, was diluted into unlabeled mixed micelles. The half-times for transfer of a homologous series of N-NBD-PEs differing in saturated acyl chain length from 11 to 16 carbons increased with acyl chain length from 4 to 35 s. The half-times for transfer of the same N-NBD-PEs between phosphatidylcholine vesicles without taurocholate were 200-6000 times slower than those between the mixed micelles. A kinetic analysis of initial transfer rate data was used to determine the mechanistic model that best described the data. According to this analysis, the increased rate of intermicellar phospholipid transfer relative to that of intervesicular transfer is a result of (1) exchange between micelles during transient micelle collisions which is not observed between vesicles and (2) an increased rate of monomer diffusion due to a faster rate of phospholipid dissociation from mixed micelles into the water phase than from vesicles. The relative significance of dissociation from mixed micelles into the water phase than from vesicles. The relative significance of collision-dependent versus monomer diffusion transfer increases with acyl chain length and hydrophobicity.