Evidence for a regular distribution of cholesterol in phospholipid bilayers from diphenylhexatriene fluorescence.

Cholesterol/dimyristoylphosphatidylcholine (DMPC) multilamellar vesicles were studied by steady-state fluorescence using diphenylhexatriene (DPH) as a probe. A series of dips were found in the plot of DPH fluorescence intensity versus cholesterol concentration at certain specific cholesterol concentrations. This observation indicates that there are dominant domains in which cholesterol molecules are regularly distributed on a hexagonal superlattice in the acyl chain matrix of DMPC at critical cholesterol concentrations. These concentrations can be predicted by an equation or a mathematical series, except the one at 33 mol %. These dips of DPH fluorescence intensity are temperature dependent. The excellent agreement between experimental data and calculated values as well as similar previous findings of dips and/or kinks in the excimer-over-monomer fluorescence in pyrenephosphatidylcholine/phospholipid mixtures confirm our conclusion about lateral organizations of cholesterol and acyl lipid chains in cholesterol/phospholipid multilamellar vesicles. The regular distribution model at critical concentration is consistent with the phase diagram of cholesterol/DMPC. Using the model of regular distribution, the physical origin of the liquid-disordered (Ld) phase, liquid-ordered phase (Lo), and coexistence of liquid-disordered phase and Lo phase (Lo + Ld) is discussed on the molecular level.     

Fluorescent Probes DPH,TMA-DPH and C17-HC Induce Erythrocyte Exovesiculation

An experimental approach has been developed to study human erythrocyte vesiculation, using the fluorescent probes diphenylhexatriene (DPH), trimethylamino-diphenylhexatriene (TMA-DPH) and heptadecyl-hydroxycoumarin (C17-HC). Acetylcholinesterase (AChE) enzyme activity measurements confirmed the presence of exovesicles released from erythrocyte membranes labeled with DPH, TMA-DPH or C17-HC. The fluorescence intensity and anisotropy values obtained showed that the amphiphilic probes TMA-DPH and C17-HC are preferentially incorporated in the exovesicles (when compared with DPH). There is a significant decrease of the cholesterol content of the exovesicle suspensions with time, independently of the fluorescence probe used, reaching undetectable cholesterol levels for the samples incubated for 48 hr. The ratios between the concentration of cholesterol released in the exovesicles after 1 hr incubation with DPH, TMA-DPH or C17-HC and the probe concentration used in the incubation were 84.7, 3.82 and 0.074, respectively. The size of the released vesicles was evaluated by dynamic light scattering spectroscopy. Some hypotheses are proposed that could explain the resemblance and differences between the results obtained for erythrocytes labeled with each probe, considering the present knowledge of membrane vesiculation mechanisms, lipid microdomains (rafts), erythrocyte membrane phospholipid asymmetry and AChE inhibition by TMA-DPH and C17-HC. This work demonstrates that the fluorescent probes DPH, TMA-DPH and C17-HC induce rapid erythrocyte exovesiculation; their use can lead to new methodologies for the study of this still poorly understood mechanism.     

A photophysical model for diphenylhexatriene fluorescence decay in solvents and in phospholipid vesicles.

The fluorescence decay of 1,6-diphenyl-1,3,5-hexatriene (DPH) in pure solvents and in phospholipid vesicles has been measured using frequency domain fluorometry. Data analysis uses a model with two energetically close excited states. The model explains the high quantum yield and the double exponential decay of DPH observed in some pure solvents and in phospholipid vesicles. This model assumes that after excitation to a first excited state, there is a rapid interconversion to a lower excited state and that most of the emission occurs from this state. The interconversion rates between the two excited states determine the average lifetime. For DPH in solvents, we find that the interconversion rates are solvent and temperature dependent. For DPH in phospholipid vesicles, we find that the back reaction rate from excited state 2 to excited state 1 (R12) is what determines the fluorescence properties. The phospholipid phase transition affects only this back reaction rate. The model was analyzed globally for a range of solvents, temperatures and vesicle composition. Of the six parameters of the model, only two, the interconversion rates between the two excited states, varied in all different samples examined. For DPH in phospholipid vesicles, there is an additional feature of the model, which is related to the apparent distribution of the rate R12. Significantly better fits were obtained using a continuous lorentzian distribution of interconversion rates. The resulting lifetime distribution was asymmetric and showed a definite narrowing above the phase transition.     

Partition coefficients of fluorescent probes with phospholipid membranes

A method for determination of membrane partition coefficients of five fluorescent membrane probes, 1,6-diphenyl-1,3,5-hexatriene (DPH), p-((6-phenyl)-1,3,5-hexatrienyl) benzoic acid (DPH carboxylic acid), 3-(p-(6-phenyl)-1,3,5-hexatrienyl)phenylpropionic acid (DPH propionic acid), 1-(4-trimethylammoniumphenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH) and N-4-(4-didecylaminostyryl)-N-methylpyridinium iodide (4-di-10-ASP), was developed utilizing the fluorescence enhancement of a constant probe concentration by titration with excess phospholipid liposomes. The partition coefficients of DPH, DPH carboxylic acid, DPH propionic acid, TMA-DPH and 4-di-10-ASP into dipalmitoylphosphatidylcholine membranes were determined to be 1.3.10(6), 1.0.10(6), 6.5.10(5), 2.4.10(5) and 2.8.10(6) respectively. Knowledge of the partition coefficients may help select a lipid concentration for membrane studies that necessitate a probe's dominant incorporation into membranes.     

Fluorescence energy transfer from diphenylhexatriene to bacteriorhodopsin in lipid vesicles

Fluorescence energy transfer between the donor diphenylhexatriene (DPH) and the acceptor retinal and fluorescence depolarization of DPH are used to test current theories for fluorescence energy transfer in two-dimensional systems and to obtain information on the effect of the intrinsic membrane protein, bacteriorhodopsin, on the order and dynamics of the lipid phase. Increasing the surface concentration of acceptors by raising the protein to lipid ratio leads to a decrease in the mean fluorescence lifetime by up to a factor of four. When the acceptor concentration is reduced at a fixed protein to lipid ratio by photochemical destruction of retinal, the lifetime increases and reaches approximately the value observed in protein-free vesicles when the bleaching is complete. The shape of the decay curve and the dependency of the mean lifetime on the surface concentration of acceptors are in agreement with theoretical predictions for a two-dimensional random distribution of donors and acceptors. From this analysis a distance of closest approach between donors and acceptors of approximately 18 A is obtained, which is close to the effective radius of bacteriorhodopsin (17 A) and consistent with current ideas about the location of retinal in the interior of the protein. In the absence of energy transfer (bleached vesicles), the steady-state fluorescence anisotropy, -r, of DPH is considerably lower than in the corresponding unbleached vesicles, indicating that the effect of energy transfer must be taken into account when interpreting -r in terms of order and dynamics.     

A new fluorimetric method to measure protein-catalyzed phospholipid transfer using 1-acyl-2-parinaroylphosphatidylcholine

A new, simple and versatile method to measure phospholipid transfer has been developed, based on the use of a fluorescent phospholipid derivative, 1-acyl-2-parinaroylphosphatidylcholine. Vesicles prepared of this phospholipid show a low level of fluorescence due to interactions between the fluorescent groups. When phospholipid transfer protein and vesicles consisting of non-labeled phosphatidylcholine are added the protein catalyzes an exchange of phosphatidylcholine between the labeled donor and non-labeled acceptor vesicles. The insertion of labeled phosphatidylcholine into the non-labeled vesicles is accompanied by an increase in fluorescence due to abolishment of self-quenching. The initial rate of fluorescence enhancement was found to be proportional to the amount of transfer protein added. This assay was applied to determine the effect of membrane phospholipid composition on the activity of the phosphatidylcholine-, phosphatidylinositol- and non-specific phospholipid transfer proteins. Using acceptor vesicles of egg phosphatidylcholine and various amounts of phosphatidic acid it was observed that the rate of phosphatidylcholine transfer was either stimulated, inhibited or unaffected by increased negative charge depending on the donor to acceptor ratio and the protein used. In another set of experiments acceptor vesicles were prepared of phosphatidylcholine analogues in which the ester bonds were replaced with ether bonds or carbon-carbon bonds. Assuming that only a strictly coupled exchange between phosphatidylcholine and analogues gives rise to the observed fluorescence increase, orders of substrate preference could be established for the phosphatidylcholine- and phosphatidylinositol transfer proteins.     

Phospholipid order in gel- and fluid-phase cell-size liposomes measured by digitized video fluorescence polarization microscopy.

Low-light digitized video fluorescence microscopy has been utilized to measure the steady-state polarized fluorescence from the membrane probe diphenylhexatriene (DPH) and its cationic and phosphatidylcholine derivatives 1-(4-trimethylammoniumphenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH) and 2-[3-(diphenylhexatrienyl)propanoyl]-3-palmitoyl-L-alpha-phosphati dylcholine (DPH-PC), respectively, in cell-size (10-70 microns) unilamellar vesicles composed of gel-or fluid-phase phospholipid. Using an inverted microscope with epi-illumination optics and an intensified silicon intensified target camera interfaced to a minicomputer, fluorescence images of single vesicles were obtained at emission polarizer orientations of 0 degrees, 45 degrees, 90 degrees, and 135 degrees relative to the excitation light polarization direction. Fluorescence intensity ratios F90 degrees/F0 degrees (= F perpendicular/F parallel) and F135 degrees/F45 degrees were calculated on a pixel-by-pixel basis from digitized image pairs. Theoretical expressions were derived for collected polarized fluorescence as a function of position on the membrane surface as well as the degree of lipid order, in terms of the fluorophore's maximum angular motional freedom in the bilayer (identical to theta max), using a modification of the method of D. Axelrod (1979. Biophys. J. 26:557-574) together with the "wobbling-in-a-cone" model of probe rotational diffusion. Comparison of experimental polarization ratios with theoretical ratios yielded the following results. In gel-phase dipalmitoyl-phosphatidylcholine, the data for all three probes correspond to a model in which the cone angle theta max = 17 +/- 2 degrees and there exists a collective tilt of the phospholipid acyl chains of 30 degrees relative to the bilayer normal. In addition, approximately 5% of DPH and TMA-DPH molecules are aligned parallel to the plane of the bilayer. In fluid-phase palmitoyloleoyl-phosphatidylcholine, the data are well fit by models in which theta max = 60 +/- 2 degrees for DPH and DPH-PC and 32 +/- 4 degrees for TMA-DPH, with approximately 20% of DPH molecules and 10% of TMA-DPH molecules aligned parallel to the bilayer plane, and a net phospholipid tilt at or near the headgroup region of approximately 30 degrees. The results demonstrate that lipid order can be measured with a spatial resolution of approximately 1 micron2 in cell-size vesicles even with high aperture observation through a microscope.     

Membrane structural domains. Resolution limits using diphenylhexatriene fluorescence decay.

Measurement of multiple fluorescence decay times of 1,6-diphenyl-1,3,5-hexatriene (DPH) in membranes can in principle be used to investigate structural domains of lipid bilayers. To assess the feasibility of this approach using phase and modulation techniques, we reduced experimental errors specifically associated with performing these measurements on membrane suspensions (probe self-quenching, background fluorescence, turbidity-induced artifacts) and determined empirically the level of precision thereby obtainable. Next we used these precision limits in theoretical calculations to conclude that the ratio of two coexisting decay times must exceed 1.3 if they are to be resolved with reliable accuracy. To demonstrate that such resolutions could be accomplished experimentally in membrane suspensions, three approaches were taken. First, the fluorescence decay of aqueous quinine sulfate quenched by chloride ion was resolved from that of membrane-associated DPH as long as the lifetime ratios of these two fluorophores exceeded the predicted value. Second, populations of DPH-containing lipid vesicles with single (or nearly single) decay times were mixed together, and when there were only two major lifetime components that differed by more than 30%, the resulting heterogeneous fluorescence could be resolved into the two expected lifetime components. Finally, DPH fluorescence decay measurements were correlated with phase behavior in well-characterized lipid systems, revealing a short lifetime component of DPH fluorescence associated with gel-phase lipid vesicles. From these studies, we conclude that only in special cases can co-existing gel and fluid phases be resolved by means of DPH lifetime heterogeneity, within the limits of precision defined herein.     

Short-lived fluorescence component of DPH reports on lipid--water interface of biological membranes

Fluorescence measurements of 1,6-diphenyl-1,3,5-hexatriene (DPH) in large unilamellar phospholipid vesicles were performed to characterize the influence of the membrane physical properties on the short-lived lifetime component of the fluorescence decay. We have found that the short-lived component of DPH significantly shortens when the membrane undergoes a temperature-induced phase transition as it is known for the long-lived component of DPH. We induced membrane phase transitions also by alcohols, which are reported to be distributed different way in the membrane–ethanol close to the membrane-water interface and benzyl alcohol in the membrane core. A different effect of the respective alcohol on the short and long decay component was observed. Both the time-resolved fluorescence spectra of DPH taken during lipid vesicle staining and the lifetime dependences caused by changes of temperature and/or induced by the alcohols show that the short-lived fluorescence originates from the population of dye molecules distributed at the membrane–water interface.     

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.     

Fluorescence lifetime and quenching studies on some interesting diphenylhexatriene membrane probes

The fluorescence lifetimes of a number of membrane probes based on the 1,6-diphenylhexatriene (DPH) chromophore have been measured in small unilamellar phospholipid vesicles and found to be multiphasic. These probes were quenched by sodium iodide with different efficiencies in vesicles and this has been attributed to the depth of the particular probe in the bilayer. The distribution of the probe between the outer and inner monolayer has been determined for those probes with fixed positions in the bilayer. The iodide ion permeability of the bilayer was found to be immeasurably small over a 3 h period.     

Lipid-phase structure in epithelial cell membranes: comparison of renal brush border and basolateral membranes

The lipid-phase structures of brush border membrane vesicles (BBMV) and basolateral membrane vesicles (BLMV) isolated from rabbit renal cortex were compared by steady-state and phase-modulation measurements of diphenylhexatriene (DPH) and trans- and cis-parinaric acid (tPnA and cPnA) fluorescence. A temperature-scanning system was used which gave reproducible temperature profiles of steady-state and dynamic fluorescence parameters with a resolution of 0.1 degrees C. Steady-state anisotropy of DPH showed a triphasic dependence on temperature with slope discontinuities at 22 +/- 4 and 47 +/- 3 degrees C (BBMV) and at 23 +/- 2 and 48 +/- 1 degrees C (BLMV). At all temperatures, DPH anisotropy in BBMV was greater than that in BLMV. Ground-state heterogeneity analysis of tPnA and cPnA fluorescence lifetime data demonstrated the presence of long (greater than 12 ns) and short (less than 5 ns) lifetime components, interpreted in terms of solid-phase and fluid-phase lipid domains. The fraction of solid-phase phospholipid decreased from 0.9 to 0.1 for BBMV and from 0.7 to 0.3 in BLMV with increasing temperature (10-50 degrees C). In both membranes, tryptophan-PnA fluorescence energy-transfer measurements showed that membrane proteins were surrounded by a fluidlike phospholipid phase. These results demonstrate the inadequacy of steady-state DPH anisotropy data in defining the structural characteristics of complex biological membranes. Results obtained with the phase-sensitive parinaric acid probes demonstrate major differences in the phase structure of the two opposing cell membranes in both the bulk lipid and the lipid microenvironment around membrane proteins.     

Evaluation of membrane phase behavior as a tool to detect extrinsic protein-induced domain formation: binding of prothrombin to phosphatidylserine/phosphatidylcholine vesicles

The temperature-composition phase diagram of mixed dimyristoylphosphatidylserine (DMPS) and dimyristoylphosphatidylcholine (DMPC) small unilamellar vesicles was determined in the presence and absence of bound bovine prothrombin by monitoring the phospholipid order-disorder phase separation using diphenylhexatriene (DPH) fluorescence anisotropy. The shape of the membrane temperature-composition diagram was essentially unaltered by the binding of prothrombin in the presence of Ca2+ although the two-phase (gel/fluid) region was slightly narrowed and shifted by 1-10 degrees C to higher temperatures. This result does not support the popular idea that extensive domains rich in negatively charged phospholipid are induced in response to prothrombin binding. Instead of implying domain formation, our results demonstrate that the observed increase in melting temperature associated with binding of prothrombin to acidic phospholipid membranes can be accounted for by the observed altered membrane order both in the fluid and in the solid lamellar phases. The membrane order in the liquid-crystalline phase increased with increased acidic lipid content, and much more so for DMPS than for dipentadecanoylphosphatidylglycerol (DC15PG). These results demonstrate that simple shifts in membrane phase behavior cannot be properly interpreted to prove the existence of charged lipid domains. In addition, we report the unexpected observation that prothrombin increased the anisotropy of DPH in DMPS/DMPC vesicles in the liquid-crystalline phase in the absence of Ca2+ as well as in its presence. This effect was seen to a lesser extent and only at a much higher charged-lipid content for DC15PG/DMPC vesicles.(ABSTRACT TRUNCATED AT 250 WORDS)     

Role of sn-1-saturated,sn-2-polyunsaturated phospholipids in control of membrane receptor conformational equilibrium: effects of cholesterol and acyl chain unsaturation on the metarhodopsin I in equilibrium with metarhodopsin II equilibrium.

The effect of phospholipid bilayer acyl chain packing free volume on the equilibrium concentration of the form of photolyzed rhodopsin which initiates visual signal transduction, metarhodopsin II (meta II), is examined in reconstituted systems formed from the saturated phospholipid dimyristoylphosphatidylcholine (DMPC) and in the polyunsaturated phospholipid sn-1-palmitoyl-sn-2-arachidonoylphosphatidylcholine (PAPC) with and without 30 mol% cholesterol. The extent of meta II formation is determined from both flash photolysis measurements and rapidly acquired absorbance spectra. Equilibrium and dynamic properties of the lipid bilayer are characterized by the dynamic fluorescence properties of 1,6-diphenyl-1,3,5-hexatriene (DPH). DPH orientational properties are characterized by fv, a parameter which reflects the volume available for probe reorientation in the bilayer, relative to that available in an unhindered, isotropic environment [Straume, M., & Litman, B. J. (1987) Biochemistry 26, 5121-5126]. The metarhodopsin I in equilibrium with meta II equilibrium constant, Keq has a linear relationship with fv for rhodopsin in PAPC vesicles with and without cholesterol as well as for rhodopsin in DMPC vesicles, and these two correlation lines have different slopes. The correlations between Keq and fv in PAPC and DMPC systems are compared with a similar correlation in the native rod outer segment disk membrane and one reported previously in an egg phosphatidylcholine (egg PC) system [Mitchell, D. C., Straume, M., Miller, J. L., & Litman, B. J. (1990) Biochemistry 29, 9143-9149].(ABSTRACT TRUNCATED AT 250 WORDS)     

Change of synaptic membrane lipid composition and fluidity by chronic administration of lithium

The effect of chronic administration of lithium salts on the lipid composition and physical properties of the synaptosomal plasma membrane was examined in rat brain. The effect of lithium treatment has been studied on the fluorescence polarization of synaptosomal plasma membrane and artificial lipid vesicles and on the lipid composition of the membranes. Fluorescence polarization of lipophilic probes was used to study membrane lipid structure. Steady-state polarization of 1,6-diphenyl-1,3,5-hexatriene (DPH), a probe of the hydrophobic core, was significantly lower in plasma membranes from lithium-treated animals. Altered DPH polarization was due to a decrease in the order parameter of the probe. The lithium-treatment also changed the fluorescence of 1-anilino-8-naphthalene sulfonate (ANS), a probe that binds to the polar head group of the phospholipids and to proteins on the membrane surface. Synaptic plasma membranes from treated rats presented no significant changes on the cholesterol-to-phospholipid ratio, although the phospholipid class distribution was altered and the membrane phospholipid unsaturation increased. In summary, the neural plasma membranes became disorder after chronic lithium administration at therapeutic levels. This structural change may be due to changes in plasma membrane phospholipid distribution and to the degree of unsaturation of phospholipid fatty acids.     

Photochemical changes of fluorescent probes in membranes and their effect on the observed fluorescence anisotropy values

The fluorescence intensity of diphenylhexatriene (DPH) and of trimethylammonium-diphenylhexatriene (TMA-DPH) is measured when these probes are embedded in vesicles of dipalmitoyl- and dioleoylphosphatidylcholine (DPPC and DOPC), in mixtures of these vesicles as well as in vesicles of the mixed phospholipids, in trout intestinal brush border membranes and in mitoplasts of rat liver cells. The intensity in DOPC vesicles is found to be significantly higher than in DPPC vesicles. When these systems are irradiated with strong ultraviolet light radiation, a decrease in the fluorescence intensity is observed; this effect is much stronger in DOPC than in DPPC vesicles. The fluorescence anisotropy values in the mixture of vesicles as well as in the membranes show an initial increase with irradiation which is followed by a significant decrease. A transfer of DPH molecules between DPPC and DOPC vesicles is observed. For TMA-DPH this transfer takes place only from DPPC to DOPC vesicles, but not vice-versa. These results are related to intensity and anisotropy measurements of these probes in cell cultures.     

Study of the interaction between the antitumour protein alpha-sarcin and phospholipid vesicles.

alpha-Sarcin is a single polypeptide chain protein which exhibits antitumour activity by degrading the larger ribosomal RNA of tumour cells. We describe the interaction of a alpha-sarcin with lipid model systems. The protein specifically interacts with negatively-charged phospholipid vesicles, resulting in protein-lipid complexes which can be isolated by ultracentrifugation in a sucrose gradient. alpha-Sarcin causes aggregation of such vesicles. The extent of this interaction progressively decreases when the molar ratio of phosphatidylcholine increases in acidic vesicles. The kinetics of the vesicle aggregation induced by the protein have been measured. This process is dependent on the ratio of alpha-sarcin present in the protein-lipid system. A saturation plot is observed from phospholipid vesicles-protein titrations. The saturating protein/lipid molar ratio is 1:50. The effect produced by the antitumour protein on the lipid vesicles is dependent on neither the length nor the degree of unsaturation of the phospholipid acyl chain. However, the aggregation is dependent on temperature, being many times higher above the phase transition temperature of the corresponding phospholipid than below it. The effects of pH and ionic strength have also been considered. An increase in the ionic strength does not abolish the protein-lipid interaction. The effect of pH may be related to conformational changes of the protein. Binding experiments reveal a strong interaction between alpha-sarcin and acidic vesicles, with Kd = 0.06 microM. The peptide bonds of the protein are protected against trypsin hydrolysis upon binding to acidic vesicles. The interaction of the protein with phosphatidylglycerol vesicles does not modify the phase transition temperature of the lipid, although it decreases the amplitude of the change of fluorescence anisotropy associated to the co-operative melting of 1,6-diphenyl-1,3,5-hexatriene (DPH)-labelled vesicles. The results are interpreted in terms of the existence of both electrostatic and hydrophobic components for the interaction between phospholipid vesicles and the antitumour protein.     

Thermotropic and dynamic characterization of interactions of acylated alpha-bungarotoxin with phospholipid bilayer membranes

The interactions of palmitoyl-alpha-bungarotoxin (PBGT) with dipalmitoylphosphatidylcholine (DPPC) bilayers have been studied by using high-sensitivity differential scanning calorimetry together with steady-state and time-resolved phosphorescence and fluorescence spectroscopy. The incorporation of PBGT into large single lamellar vesicles causes a decrease in the phospholipid phase transition temperature (Tm), a broadening of the heat capacity function, and a decrease in the enthalpy change associated with the phospholipid gel to liquid-crystalline transition. Analysis of the dependence of this decreased enthalpy change on the protein/lipid molar ratio indicates that each PBGT molecule exhibits a localized effect upon the bilayer, preventing approximately six lipid molecules from participating in the lipid phase transition. Additional calorimetric experiments indicate that binding to acetylcholine receptor enriched membranes causes a small increase in the Tm of the PBGT/DPPC vesicles. Steady-state fluorescence depolarization measurements employing 1,6-diphenyl-1,3,5-hexatriene (DPH) indicate that the association of PBGT with the phospholipid bilayer decreases the apparent order of the bulk lipid below Tm while increasing the order above Tm. These results have been further supported by rotational mobility measurements of erythrosin-labeled PBGT associated with giant (about 2-micron) unilamellar vesicles composed of dielaidoylphosphatidylcholine or dioleoylphosphatidylcholine using the time-dependent decay of delayed fluorescence/phosphorescence emission anisotropy. Rotational correlation times in the submillisecond time scale (about 30 microseconds) indicate that the protein is highly mobile in the fluid phase and that below Tm the rotational mobility is only slightly restricted.(ABSTRACT TRUNCATED AT 250 WORDS)     

Effects of ethanol on lipid bilayers with and without cholesterol: the distearoylphosphatidylcholine system

Differential scanning calorimetry (DSC) and fluorescence spectroscopy are useful techniques for investigating the phase transitions of phospholipid bilayers. In this study, these methods have been extended to determine the effects of ethanol on DSPC and DSPC/2 mol.% cholesterol bilayers. The biphasic effect of the main transition was observed on the DSC heating scans above 0.60 M ethanol. In addition, the concentration at which the biphasic effect occurs is not significantly changed in the presence of 2 mol.% cholesterol. For the fluorescence studies, 1,6-diphenyl-1,3,5-hexatriene (DPH) has been incorporated into the bilayer to monitor the phase transitions through the displacement of DPH. This fluorescent probe is used to directly determine the onset of interdigitation in the bilayer systems as indicated by a large decrease in the DPH fluorescence intensity. The addition of cholesterol lowered and broadened the transition temperatures of the phosphatidylcholine (PC) system. However, 2 mol.% cholesterol did not have a significant effect on the induction of the interdigitated phase in DSPC as observed from the small difference in ethanol threshold concentration for the two systems. This suggests that DSPC forms a more stable interdigitated gel phase than other PCs with shorter acyl chains.     

Effect of proteins on fluorophore lifetime heterogeneity in lipid bilayers.

The effect of three different membrane proteins on the fluorescence lifetime heterogeneity of 1,6-diphenyl-1,3,5-hexatriene (DPH) in phospholipid vesicle systems was investigated. For large unilamellar vesicles of dimyristoylphosphatidylcholine (DMPC) and 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) at 37 degrees C, the fluorescence decay was essentially monoexponential (8.6 and 8.2 ns, respectively) except for a minor component typical of DPH. For gramicidin D reconstituted into DMPC vesicles at a protein/lipid molar ratio of 1/7, the most appropriate analysis of the data was found to be in the form of a bimodal Lorentzian distribution. Centers of the major lifetime components were almost identical with those recovered for vesicles without proteins, while broad distributional widths of some 4.0 ns were recovered. Variation of the protein/lipid molar ratio in sonicated POPC vesicles revealed an abrupt increase in distributional width at ratios approximating 1/15-1/20, which leveled off at about 2.5 ns. For bacteriorhodopsin in DMPC vesicles and cytochrome b5 in POPC, the most appropriate analysis of the data was again found to be in the form of a bimodal Lorentzian also with broad distributional widths in the major component. Lifetime centers were decreased for these proteins due to fluorescence energy transfer to the retinal of the bacteriorhodopsin and heme of the cytochrome b5. Fluorescence energy transfer is distance dependent, and since a range of donor-acceptor distances would be expected in a membrane, lifetime distributions should therefore be recovered independently of other effects for proteins possessing acceptor chromophores.(ABSTRACT TRUNCATED AT 250 WORDS)