Fluorescence properties of cholestatrienol in phosphatidylcholine bilayer vesicles

The fluorescent sterol delta 5,7,9,(11)-cholestatrien-3 beta-ol (cholestatrienol) was incoporated into 1-palmitoyl-2-oleoyl-phosphatidylcholine (POPC) small unilamellar vesicles (SUV) with and without cholesterol in order to monitor sterol-sterol interactions in model membranes. Previously another fluorescent sterol, dehydroergosterol (F. Schroeder, Y. Barenholz, E. Gratton and T.E. Thompson. Biochemistry 26 (1987) 2441), was used for this purpose. However, there is some concern that dehydroergosterol may not be the best analogue for cholesterol. Fluorescence properties of cholestatrienol in POPC SUV were highly sensitive to cholestatrienol purity. The fluorescence decay of cholestatrienol in the POPC SUV was analyzed by assuming either that the decay is comprised of a discrete sum of exponential components or that the decay is made up of one or more component's distribution of lifetimes. The decay for cholestatrienol in POPC SUV analyzed using distributions had a lower chi 2 value and was described by a two-component Lorentzian function with centers near 0.86 and 3.24 ns, and fractional intensities of 0.96 and 0.04, respectively. Both distributions were quite narrow, i.e., 0.05 ns full-width at half-maximum peak height. It is proposed that the two lifetime distributions are generated by separate continua of environments for the cholestatrienol molecule described by different dielectric constants. In the range 0-6 mol% cholestatrienol, the cholestatrienol underwent a concentration-dependent relaxation. This process was characterized by red-shifted absorption and maxima and altered ratios of absorption and fluorescence excitation maxima. Fluorescence quantum yield, lifetime, steady-state anisotropy, limiting anisotropy and rotational rate remained constant. In contrast, in POPC vesicles containing between 6 and 33 mol% cholestatrienol, the fluorescent cholestatrienol partially segregated, resulting in quenching. Thus, below 6 mol% cholestatrienol, the cholestatrienol appeared to behave in part as monomers exposed to some degree to the aqueous solvent in a sterol-poor domain within POPC bilayers. Since the lifetime did not decrease above 6 mol% cholestatrienol, the fluorescence at high mol% values of cholestatrienol was due to cholestatrienol in the sterol-poor domain. The fluorescence intensity, quantum yield, steady-state anisotropy, and limiting anisotropy of cholestatrienol in the sterol-poor domain decreased to limiting, nonzero values while the rotational rate increased to a limiting value. Thus, the sterol-poor domain became more disordered when it coexisted with the sterol-rich domain.(ABSTRACT TRUNCATED AT 400 WORDS)     

Time-resolved fluorescence investigation of membrane cholesterol heterogeneity and exchange

The fluorescent sterol delta 5,7,9(11),22-ergostatetraen-3 beta-ol (dehydroergosterol) was investigated as a cholesterol analogue to examine sterol domains in and spontaneous exchange of sterol between 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) small unilamellar vesicles (SUV). Fluorescence lifetime, acrylamide quenching analyses, and intermembrane exchange kinetics were consistent with the presence of at least two sterol domains in POPC. Fluorescence lifetime was determined by phase and modulation fluorescence spectroscopy and analyzed by nonlinear least-squares as well as continuous distributional analyses. Both methods demonstrated that pure dehydroergosterol in POPC SUV had two lifetime components (C) and fractional intensities (F) near C1 = 0.851 ns (F1 0.96) and C2 = 2.668 ns (F2 0.004). In contrast to component C1, the center of lifetime distribution, fractional intensity, and peak width of dehydroergosterol lifetime component C2 was dependent on the polarity of the medium and vesicle curvature. The sterol domain corresponding to dehydroergosterol component C2 was preferentially quenched by acrylamide. Acrylamide quenching of dehydroergosterol fluorescence demonstrated that the two lifetime components of dehydroergosterol were not due to transbilayer sterol domains with different lifetimes. In a spontaneous exchange assay not requiring separation of donor and acceptor SUV, the lifetime component C2, but not C1, shifted to a shorter lifetime with altered distributional width. The kinetics of these lifetime and distributional width changes best fitted a two-exponential function, with a fast exchange rate constant K1 = 0.0325 min-1, t1/2 = 21.3 min, and a slow rate constant k2 = 0.00275 min-1, t1/2 = 261 min. The fast exchanging pool correlates with the longer lifetime component C2. These kinetics were confirmed both by dehydroergosterol exchange measured with fluorescence intensity and by [3H]cholesterol exchange. In summary, lifetime, distributional width, acrylamide quenching, and classical exchange assay data are consistent with the presence of at least two pools of sterol in POPC SUV.     

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)     

Fluorescence lifetime distributions of parinaroyl phospholipids in choline plasmalogen and phosphatidylcholine bilayers containing different amounts of cholesterol

The fluorescence decay of alkenylparinaroyl- and palmitoylparinaroyl glycerophosphocholines in vesicles of the unlabeled alkenyloleoyl and palmitoyloleoyl analogs was determined by multifrequency phase and modulation fluorometry. The measured phase angles and demodulations could be equally well fitted to a biexponential decay, as well as unimodal or bimodal continuous lifetime distributions. The latter model was applied to study the influence of cholesterol on parinaroyl phospholipid fluorescence in vesicles. The long-living component of a bimodal lifetime distribution was sensitive toward the presence of the sterol. Upon increasing cholesterol concentrations, its lifetime center increased and its distribution widths decreased. Lifetime distribution widths in vesicles of alkenyloleoyl- or palmitoyloleoyl-glycerophosphocholine (choline plasmalogen and phosphatidylcholine, respectively) were reduced by the sterol to the same extent. We interprete the sterol-induced lifetime distribution narrowing as an effect due to an increase of membrane homogeneity in cholesterol-phospholipid membranes.     

A fluorescence study of dehydroergosterol in phosphatidylcholine bilayer vesicles

The fluorescent sterol delta 5,7,9(11),22-ergostatetraen-3 beta-ol (dehydroergosterol) was incorporated into 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) small unilamellar vesicles (SUV) with and without cholesterol in order to monitor sterol-sterol interactions in model membranes. In the range 0-5 mol % fluorescent sterol, dehydroergosterol underwent a concentration-dependent relaxation characterized by red-shifted wavelengths of maximum absorption as well as altered ratios of absorbance maxima and fluorescence excitation maxima at 338 nm/324 nm. Fluorescence intensity per mole of dehydroergosterol increased up to 5 mol % in POPC vesicles. In contrast, quantum yield, steady-state anisotropy, limiting anisotropy, lifetime, and rotational rate remained relatively constant in this concentration range. Similarly, addition of increasing cholesterol in the range 0-5 mol % in the presence of 3 mol % dehydroergosterol also increased the fluorescence intensity per mole of dehydroergosterol, red-shifted wavelengths of maximum absorption, and altered ratios of absorbance maxima. In POPC vesicles containing between 5 and 33 mol % dehydroergosterol, the fluorescent dehydroergosterol interacted to self-quench, thereby decreasing the fluorescence intensity, quantum yield, steady-state anisotropy, and limiting anisotropy and increasing the rotational rate (decreased rotational relaxation time) of the fluorescent sterol. The fluorescence lifetime of dehydroergosterol remained unchanged. The results were in accord with the interpretation that below 5 mol% sterol, the sterols behaved as monomers exposed to some degree to the aqueous solvent in POPC bilayers.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fluorescence lifetime distributions of 1,6-diphenyl-1,3,5-hexatriene in phospholipid vesicles

The fluorescence emission properties of 1,6-diphenyl-1,3,5-hexatriene (DPH) in 1,2-dipalmitoyl-3-sn-phosphatidylcholine and 1,2-dimyristoyl-3-sn-phosphatidylcholine multilamellar vesicles have been measured by using multifrequency phase fluorometry. The fluorescence decay of DPH in the phospholipid vesicles has been analyzed by assuming either that the decay is made up of a discrete sum of exponential components or that the decay is made up of one or more continuous distributions of lifetime components. The fit of the decay curve using exponentials required at least two terms, and the reduced X2 was relatively large. The fit using a continuous distribution of lifetime values used two continuous components. Several symmetric distribution functions were used: uniform, Gaussian, and Lorentzian. The distribution function that best described the decay was the Lorentzian. The full width at half-maximum of the Lorentzian distribution was about 0.6 ns at temperatures below the phase transition temperature. At the phospholipid phase transition and at higher temperatures, the distribution became quite narrow, with a width of about 0.1 ns. It is proposed that the lifetime distribution is generated by a continuum of different environments of the DPH molecule characterized by different dielectric constants. Below the transition temperature in the gel phase, the dielectric constant gradient along the membrane normal determines the distribution of decay rates. Above the transition, in the liquid-crystalline phase, the translational and rotational mobility of the DPH molecule increases, and the DPH experiences an average environment during the excited-state lifetime. Consequently, the distribution becomes narrower.(ABSTRACT TRUNCATED AT 250 WORDS)     

Organization and interaction of cholesterol and phosphatidylcholine in model bilayer membranes

The molecular organization of sterols in liposomes of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) at 37 degrees C is examined by utilizing the fluorescent analogue of cholesterol cholesta-5,7,9-trien-3 beta-ol (cholestatrienol). (1) Cholestatrienol is shown to be indistinguishable from native cholesterol in terms of its ability to condense POPC, as determined by (i) pressure/area studies of mixed-lipid monolayers and (ii) its ability to increase the order of POPC bilayers (determined by electron spin resonance studies) whether on its own or admixed with cholesterol at various ratios. (2) By analysis of the perturbation of the absorption spectra, cholestatrienol was found to be freely miscible in aggregates of cholesterol in buffer. In contrast, a lack of any detectable direct interaction of the sterol molecules in POPC bilayers was detected. (3) Fluorescence intensity and lifetime measurements of POPC/sterol (1:1 mol/mol) at various cholesterol/cholestratrienol molar ratios (0.5:1 up to 1:1 cholestatrienol/POPC) confirmed that sterol molecules in the membrane matrix were not associated to any great degree. (4) A quantitative estimate of how close sterol molecules approach each other in the membrane matrix was evaluated from the concentration dependence of the steady-state depolarization of fluorescence and was found to be 10.6 A. From geometrical considerations, the sterol/phospholipid phase at 1:1 mol/mol is depicted as each sterol having four POPC molecules as nearest neighbors. We term this arrangement of the lipid matrix an "ordered bimolecular mesomorphic lattice". (5) The concentration dependence of depolarization of fluorescence of cholestatrienol in POPC liposomes in the absence of cholesterol yielded results that were consistent with the cholestatrienol molecules being homogeneously dispersed throughout the phospholipid phase at sterol/POPC ratios of less than 1:1. (6) From qualitative calculations of the van der Walls' hydrophobic interactions of the lipid species, the phospholipid condensing effect of cholesterol is postulated to arise from increased interpenetration of the flexible methylene segments of the acyl chains, as a direct result of their greater mutual attraction compared to their attraction for neighboring sterol molecules. (7) The interdependence of the ordered bimolecular mesomorphic lattice and the acyl chain condensation is discussed in an effort to understand the ability of cholesterol to modulate the physical and mechanical properties of biological membranes.     

Properties influencing fluorophore lifetime distributions in lipid bilayers

The fluorescence lifetime of the membrane fluorophore 1,6-diphenyl-1,3,5-hexatriene has been analyzed according to the distributional approach in a number of lipid bilayer systems. The systems included vesicles of 16:0/18:1-phosphatidylcholine (POPC), egg phosphatidylcholine (EYPC), microsomal phospholipids, and also intact microsomal membranes. With increasing complexity of composition, an increasingly broader width was found in the major component of a bimodal Lorentzian fluorescence lifetime distribution. In order to explain these findings, we propose a model based on environmental heterogeneity and environmental sampling, where the environment is defined as the lipid molecules immediately surrounding the fluorophore. Environmental heterogeneity is thought of as arising from organizational, compositional, and solvent factors. Environmental sampling pertains to the ability of a fluorophore to detect environments in a system and is a function of the fluorophore lifetime and the lipid dynamics. If the fluorescence lifetime is sufficiently short, the fluorophore will only sample a particular environment, and great compositional complexity will mean that each fluorophore in an ensemble will decay to the ground state with a different time. This appears to explain why in our results with DPH a narrow width is obtained for POPC, where vesicles are composed of a single phospholipid molecular species, compared to EYPC and microsomal phospholipid vesicles having complex molecular species composition. This model should serve as a basis for understanding the interrelationships of environmental complexity and lipid dynamics in membranes.     

Fluorescence studies of the conformational dynamics of parvalbumin in solution: lifetime and rotational motions of the single tryptophan residue

The fluorescence properties of the single tryptophan residue in whiting parvalbumin were used to probe the dynamics of the protein matrix. Ca2+ binding caused a blue-shift in the emission (from lambda max = 339 to 315 nm) and a 2.5-fold increase in quantum yield. The fluorescence decay was nonexponential in both Ca2(+)-free and Ca2(+)-bound parvalbumin and was best described by Lorentzian lifetime distributions centered around two components: a major long-lived component at 2-5 ns and a small subnanosecond component. Raising the temperature from 8 to 45 degrees C resulted in a decrease in both the center (average) and width (dispersion) of the major lifetime distribution component, whereas the center, width, and fractional intensity of the fast component increased with temperature. Arrhenius activation energies of 1.3 and 0.3 kcal/mol were obtained in the absence and in the presence of Ca2+, respectively, from the temperature dependence of the center of the major lifetime distribution component. Direct anisotropy decay measurements of local tryptophan rotations yielded an activation energy of 2.3 kcal/mol in Ca2(+)-depleted parvalbumin and indicated a correlation between rotational rates and lifetime distribution parameters (center and width). Ca2+ binding produced a decrease in the width of the major lifetime distribution component and a decrease in tryptophan rotational mobility within the protein. There was a rough correlation between these two parameters with changes in Ca2+ and temperature, so that both measurements may be taken to indicate that the structure of Ca2(+)-bound parvalbumin was more rigid than in Ca2(+)-depleted parvalbumin.     

Increased membrane heterogeneity in stimulated human granulocytes

TMA-DPH fluorescence decay in human PMN before and after stimulation with FMLP was studied using frequency domain fluorometry. Membrane heterogeneity was assessed by the width of the continuous distributions of lifetime values of Lorentzian shape used to describe the fluorescence decay. In non-stimulated granulocytes TMA-DPH fluorescence decay is characterized by two distributions of lifetime values centered at 6.5 and 1.0 ns and full width at half maximum of 0.3 and 1.2 ns, respectively. Within 15 min after stimulation, the center values of the two distribution components were 5.1 and 0.8 ns and the distribution width was 0.8 and 0.6 ns, respectively. These results indicate changes of membrane domain organization which can be ascribed to compositional changes and redistribution of membrane components.     

Fluorescence lifetime distribution of 1,8-anilinonaphthalenesulfonate (ANS) in reversed micelles detected by frequency domain fluorometry.

The fluorescence emission decay of ANS (1,8-anilinonaphthalenesulfonate) in reversed AOT (sodium bis-(2-ethyl-1-hexy)sulfosuccinate) micelles at different water contents was investigated by frequency domain fluorometry. The whole ANS emission decay in reversed AOT micelles could not be fitted in terms of discrete lifetime values, i.e., mono-exponential and bi-exponential models. Better fits were obtained when using continuous unimodal Lorentzian lifetime distributions. This was interpreted as arising from the reorientation processes of water molecules around the excited state of ANS or probe exchange among different probe locations, occurring on a time scale longer than fluorophore lifetime. The dependence of ANS fluorescence anisotropy on the emission wavelength was consistent with the existence of a great emission heterogeneity especially for inverted micelles having reduced H2O/AOT molar ratio. Finally, the observation that the distribution width decreases with increasing temperature and/or micelle size suggested that fast processes of water dipolar reorganization around the fluorophore are facilitated under these conditions.     

Multiple conformational states in myoglobin revealed by frequency domain fluorometry

The tryptophanyl fluorescence decays of two myoglobins, i.e., sperm whale and tuna myoglobin, have been examined in the frequency domain with an apparatus which utilizes the harmonic content of a mode-locked laser. Data analysis was performed in terms of continuous distribution of lifetime having a Lorentzian shape. Data relative to sperm whale myoglobin, which possesses two tryptophanyl residues, i.e., Trp-A-5 and -A-12, provided a broad lifetime distribution including decay rates from a few picoseconds to about 10 ns. By contrast, the tryptophanyl lifetime distribution of tuna myoglobin, which contains only Trp-A-12, showed two well-separated and narrow Lorentzian components having centers at about 50 ps and 3.37 ns, respectively. In both cases, the chi 2 obtained from distribution analysis was lower than that provided by a fit using the sum of exponential components. The long-lived components present in the fluorescence decay of the two myoglobins do not correspond to any of those observed for the apoproteins at neutral pH. The tryptophanyl lifetime distribution of sperm whale apomyoglobin consists of two separated Lorentzian components centered at 2.25 and 5.4 ns, whereas that of tuna apomyoglobin consists of a single Lorentzian component, whose center is at 2.19 ns. Acidification of apomyoglobin to pH 3.5 produced a shift of the distribution centers toward longer lifetimes.(ABSTRACT TRUNCATED AT 250 WORDS)     

A fluorescence and radiolabel study of sterol exchange between membranes

The fluorescent sterols delta 5,7,9(11),22-ergostatetraen-3 beta-ol (dehydroergosterol) and delta 5,7,9,(11)-cholestatrien-3 beta-ol (cholestatrienol) as well as [1,2-3H]cholesterol were utilized as cholesterol analogues to examine spontaneous exchange of sterol between 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) small unilamellar vesicles (SUV). Exchange of fluorescent sterols was monitored at 24 degrees C by release from self-quenching of polarization from the time of mixing without separation of donor and acceptor vesicles. The polarization curve for 35 mol% sterol in POPC best fitted a two-exponential function, with a fast-exchange rate constant k1 = 0.0217 min-1, 1t1/2 = 32 min, size pool 1 = 12%, and a slow rate constant k2 = 2.91.10(-3) min-1, 2t1/2 = 238 min, size pool 2 = 88%. In addition to the above two exchangeable pools of sterol, the data were consistent with the presence of a slowly or nonexchangeable pool, 42% of total sterol, that was highly dependent on sterol content. These results were confirmed by simultaneous monitoring of [1,2-3H]cholesterol radioactivity and dehydroergosterol fluorescence intensity after separation of donor and acceptor vesicles by ion-exchange column chromatography. Thus, dehydroergosterol or cholestatrienol exchange as measured by fluorescence parameters (polarization and/or intensity) provides two new methods to follow cholesterol spontaneous exchange. These methods allow resolution and quantitation of a shorter exchange t1/2 near 30 min previously not reported. Thus, the cholesterol desorption rate from membranes may be faster than previously believed. In addition, the presence of a slowly non-exchangeable pool was confirmed.     

Effect of hydrostatic pressure on water penetration and rotational dynamics in phospholipid-cholesterol bilayers.

The effect of high hydrostatic pressure on the lipid bilayer hydration, the mean order parameter, and rotational dynamics of 1,2-dipalmitoyl-sn-glycero-3-phosphocholine (DPPC) and 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) cholesterol vesicles has been studied by time-resolved fluorescence spectroscopy up to 1500 bar. Whereas the degree of hydration in the lipid headgroup and interfacial region was assessed from fluorescence lifetime data using the probe 1-(4-trimethylammonium-phenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH), the corresponding information in the upper acyl chain region was estimated from its effect on the fluorescence lifetime of and 3-(diphenylhexatrienyl)propyl-trimethylammonium (TMAP-DPH). The lifetime data indicate a greater level of interfacial hydration for DPPC bilayers than for POPC bilayers, but there is no marked difference in interchain hydration of the two bilayer systems. The addition of cholesterol at levels from 30 to 50 mol% to DPPC has a greater effect on the increase of hydrophobicity in the interfacial region of the bilayer than the application of hydrostatic pressure of several hundred to 1000 bar. Although the same trend is observed in the corresponding system, POPC/30 mol% cholesterol, the observed effects are markedly less pronounced. Whereas the rotational correlation times of the fluorophores decrease in passing the pressure-induced liquid-crystalline to gel phase transition of DPPC, the wobbling diffusion coefficient remains essentially unchanged. The wobbling diffusion constant of the two fluorophores changes markedly upon incorporation of 30 mol% cholesterol, and increases at higher pressures, also in the case of POPC/30 mol% cholesterol. The observed effects are discussed in terms of changes in the rotational characteristics of the fluorophores and the phase-state of the lipid mixture. The results demonstrate the ability of cholesterol to adjust the structural and dynamic properties of membranes composed of different phospholipid components, and to efficiently regulate the motional freedom and hydrophobicity of membranes, so that they can withstand even drastic changes in environmental conditions, such as high external hydrostatic pressure.     

Saturation with cholesterol increases vertical order and smoothes the surface of the phosphatidylcholine bilayer: a molecular simulation study

Molecular dynamics (MD) simulations of a mono-cis-unsaturated 1-palmitoyl-2-oleoyl-phosphatidylcholine (POPC) bilayer and a POPC bilayer containing 50mol% cholesterol (POPC-Chol50) were carried out for 200ns to compare the spatial organizations of the pure POPC bilayer and the POPC bilayer saturated with Chol. The results presented here indicate that saturation with Chol significantly narrows the distribution of vertical positions of the center-of-mass of POPC molecules and POPC atoms in the bilayer. In the POPC-Chol50 bilayer, the same moieties of the lipid molecules are better aligned at a given bilayer depth, forming the following clearly separated membrane regions: the polar headgroup, the rigid core consisting of steroid rings and upper fragments of the acyl chains, and the fluid hydrocarbon core consisting of Chol chains and the lower fragments of POPC chains. The membrane surface of the POPC-Chol50 bilayer is smooth. The results have biological significance because the POPC-Chol50 bilayer models the bulk phospholipid portion of the fiber-cell membrane in the eye lens. It is hypothesized that in the eye lens cholesterol-induced smoothing of the membrane surface decreases light-scattering and helps to maintain lens transparency.     

Dependence on phospholipid composition of the fraction of cholesterol undergoing spontaneous exchange between small unilamellar vesicles

Spontaneous cholesterol exchange between small unilamellar vesicles comprised of different phospholipids and their binary mixtures has been studied in order to understand the factors involved in the establishment and maintenance of intracellular cholesterol distributions. Exchange was performed from neutral donor vesicles containing different cholesterol concentrations, traces of [3H]cholesterol, and [14C]cholesteryl oleate as a nonexchangeable marker. The acceptor vesicles, in 10-fold excess, had the same composition, but 15 mol % phosphatidylglycerol was included to permit chromatographic separation. Data were best fitted by a single exponential and a base value. In donor vesicles containing only one phospholipid, the kinetic rate constants agreed with data reported previously; however, the base values were larger than the expected equilibrium value of 9.09%. The size of this nonexchangeable pool and the exchange rate were found to depend on the type of phospholipid. In binary phospholipid donor systems, well above the transition temperatures of the lipid components, the exchange parameters were preferentially closer to those of one component according to the order POPC greater than DMPC greater than DPPC greater than bovine brain SPM.     

Influence of stigmastanol and stigmastanyl-phosphorylcholine, two plasma cholesterol lowering substances, on synthetic phospholipid membranes. A 2H- and 31P-NMR study.

Cholesterol, stigmastanol, and stigmastanyl-phosphorylcholine (ST-PC) were incorporated into model membranes composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) or 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC). POPC and ST-PC were deuterated at the lipid headgroup, DOPC at the cis-double bonds. The influence of the three sterols on the motion and conformation of the lipid headgroups and the hydrocarbon chains was monitored with 2H- and 31P-NMR. All three sterols were freely miscible with the lipid matrix in concentrations of up to 50 mol% without inducing phase separations or nonbilayer structures. However, the molecules exert quite different effects on the phospholipid bilayer. Cholesterol and stigmastanol are largely buried in the hydrocarbon part of the membrane, distinctly restricting the flexing motions of the fatty acyl chains whereas the conformation of the phospholipid headgroups is little affected. In contrast, ST-PC is anchored with its headgroup in the layer of phospholipid dipoles, preventing an extensive penetration of the sterol ring into the hydrocarbon layer. Hence ST-PC has almost no effect on the hydrocarbon chains but induces a characteristic conformational change of the phospholipid headgroups. The 2H- and 31P-NMR spectra of mixed phospholipid/ST-PC membranes further demonstrate that the PC headgroup of ST-PC has a similar orientation as the surrounding phosphatidylcholine headgroups. For both types of molecules the -P-N+ dipole is essentially parallel to the membrane surface. Addition of ST-PC induces a small rotation of the POPC headgroup towards the water phase.     

Time-resolved fluorescence of erythrocyte plasma membrane Ca2(+)-ATPase in different functional states.

The fluorescence decay of the plasma membrane calmodulin-activated Ca2(+)-ATPase from the erythrocyte was measured for the first time. The availability of a novel procedure for on-line blank subtraction in frequency-domain lifetime data acquisition (G.G. Reinhart, B. Feddersen, D. Jameson and E. Gratton, Biophys. J. 57 (1990) 189a) permitted the elimination of background interference from detergent-solubilized purified plasma membrane ATPase samples. The fluorescence decay of the erythrocyte Ca2(+)-ATPase was measured in the absence of Ca2+, or in the presence of Ca2+ or Ca2+ plus calmodulin. In the three different experimental conditions the fluorescence decay was very heterogeneous and could be best described by Lorentzian distributions of lifetime values. In the absence of Ca2+ the decay was described by a broad lifetime distribution centered at 4.4 ns with a width of 3.2 ns, indicating heterogeneity of tryptophan microenvironments in the ATPase. Calcium ion binding promoted an 11% increase in the center and a 27% decrease in the width of the distribution. By contrast, addition of calmodulin in the presence of Ca2+ caused a 15% decrease in the center of the distribution, revealing structural difference between calmodulin-activated and Ca2(+)-activated states of the ATPase. These results indicate the usefulness of on-line blank subtraction in frequency-domain lifetime measurements to investigate conformational changes in detergent-solubilized membrane protein samples.     

Role of sterol superlattice in free radical-induced sterol oxidation in lipid membranes

We developed a new fluorescence assay for sterol oxidation and used it to study the relationship between free radical-induced sterol oxidation and membrane sterol lateral organization. This assay used dehydroergosterol (DHE) as both a membrane probe and a membrane component. Sterol oxidation was induced by a free radical generator, AAPH (2,2'-azobis(2-amidinopropane)dihydrochloride). Using this new assay, we found that, in unilamellar vesicles composed of DHE and 1-palmitoyl-2-oleoyl-l-alpha-phosphatidylcholine (POPC), the initial rate of DHE oxidation induced by AAPH changed with membrane sterol content in an alternating manner, exhibiting a local maximum at 20.3, 22.2, 25.0, 32.3, and 40.0 mol % DHE. These mole fractions correspond to the critical sterol mole fractions C(r) predicted for maximal sterol superlattice formation. In three-component bilayers composed of POPC, cholesterol, and DHE (fixed at 1 and 5 mol %), the initial rate of AAPH-induced DHE oxidation exhibited a biphasic change whenever the total sterol mole fraction, irrespective of the DHE content, was near C(r), indicating that the correlation between sterol oxidation and sterol superlattice formation revealed in this study is not an artifact due to the use of the fluorescent cholesterol analogue DHE. The alternating variation of AAPH-induced sterol oxidation with sterol content also appeared in multicomponent unilamellar vesicles containing bovine brain sphingomyelins (bbSPM), POPC, and DHE. The present work and our previous study on cholesterol oxidase-induced sterol oxidation [Wang et al. (2004) Biochemistry 43, 2159-2166] suggest that sterol oxidation in general, either by reactive oxygen species or by enzymes, may be regulated by the extent of sterol superlattice in the membrane and thus regulated by the membrane sterol content in a fine-tuning manner.     

Interaction of lysophospholipid/taurodeoxycholate submicellar aggregates with phospholipid bilayers.

The equilibrium partitioning and the rate of transfer of monoacylphosphatidylethanolamines (lysoPEs) between phospholipid bilayers and lysoPE/taurodeoxycholate submicellar aggregates (SMAs) were examined with a series of environment-sensitive fluorescent-labeled N-(7-nitro-2,1,3-benzoxadiazol-4-yl)-1-monoacylphosphatidyletha nolamine (N-NBD-lysoPE) probes of differing acyl chain length. Our previous work has demonstrated the formation of SMAs between bile salts and lysophospholipids [Shoemaker & Nichols (1990) Biochemistry 29, 5837-5842]. The experiments in the current work demonstrate that SMAs can coexist with phospholipid vesicles and can function as shuttle carriers for the transfer of lysophospholipids between membranes. The formation of submicellar aggregates of N-NBD-lysoPE and taurodeoxycholate (TDC) in equilibrium with 1-palmitoyl-2-oleoylphosphatidylcholine (POPC) vesicles was determined from the increase in fluorescence generated upon addition of TDC to POPC vesicles containing 3 mol% N-NBD-lysoPE and 3 mol% N-(lissamine rhodamine B sulfonyl)dioleoylphosphatidylethanolamine (N-Rh-PE) as a nonextractable fluorescence energy-transfer quencher. The fraction of lysolipid extracted increased as a function of decreasing acyl chain length of the N-NBD-lysoPE molecule. The half-time for equilibration was independent of acyl chain length and averaged 44 ms at 10 degrees C. The delivery of N-NBD-lysoPE from preformed N-NBD-lysoPE/TDC SMAs into POPC vesicles containing the energy-transfer quencher N-Rh-PE was measured by the rate of fluorescence decline. The initial rate of insertion increased with decreasing acyl chain length of the N-NBD-lysoPE molecule and as a function of vesicle concentration.(ABSTRACT TRUNCATED AT 250 WORDS)