Phosphatidic acid affects structural organization of phosphatidylcholine liposomes. A study of 1,6-diphenyl-1,3,5-hexatriene (DPH) and 1-(4-trimethylammonium-phenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH) fluorescence decay using distributional analysis

The fluorescence decay of 1-(4-trimethylammonium-phenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH) was used to study micro-heterogeneity of 1,2-dimyristoyl-3-sn-phosphatidylcholine (DMPC) liposomes and to characterize the effect of phosphatidic acid on the correlation between fluorescence microheterogeneity and membrane permeability. The fluorescence decay, measured using multifrequency phase fluorometry, has been analyzed either by using a model of discrete exponential components or a model of continuous distribution of lifetime values. Both analyses have shown that TMA-DPH decay is characterized by two components: a long one of about 9 ns and a short one of about 5 ns. In the gel phase, at variance with previous DPH studies, the short component was associated with a large fractional intensity. The distributional analysis showed changes of lifetime values and width in correspondence to the calorimetric transitions. The presence of egg phosphatidic acid increased both long lifetime values and distributional width. The use of TMA-DPH as a probe to evaluate membrane heterogeneity using the distributional width is discussed. The effect of phosphatidic acid on the membrane surface and in the hydrophobic core has been related to its structural properties and to its role in water penetration.     

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)     

Resolvability of fluorescence lifetime distributions using phase fluorometry.

The analysis of the fluorescence decay using discrete exponential components assumes that a small number of species is present. In the absence of a definite kinetic model or when a large number of species is present, the exponential analysis underestimates the uncertainty of the recovered lifetime values. A different approach to determine the lifetime of a population of molecules is the use of probability density functions and lifetime distributions. Fluorescence decay data from continuous distributions of exponentially decaying components were generated. Different magnitudes of error were added to the data to simulate experimental conditions. The resolvability of the distributional model was studied by fitting the simulated data to one and two exponentials. The maximum width of symmetric distributions (uniform, gaussian, and lorentzian), which cannot be distinguished from single and double exponential fits for statistical errors of 1 and 0.1%, were determined. The width limits are determined by the statistical error of the data. It is also shown that, in the frequency domain, the discrete exponential analysis does not uniformly weights all the components of a distribution. This systematic error is less important when probability and distribution functions are used to recover the decay. Finally, it is shown that real lifetime distributions can be proved using multimodal probability density functions. In the companion paper that follows we propose a physical approach, which provides lifetime distribution functions for the tryptophan decay in proteins. In the third companion paper (Alcala, J.R., E. Gratton, and F.J. Prendergast, 1987, Biophys. J., in press) we use the distribution functions obtained to fit data from the fluorescence decay of single tryptophan proteins.     

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.     

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)     

Headgroup hydration and motional order of lipids in lamellar liquid crystalline and inverted hexagonal phases of unsaturated phosphatidylethanolamine--a time-resolved fluorescence study

By the use of frequency domain cross-correlation fluorometry, the fluorescence lifetime of the water soluble probe 8,1-anilinonapthalene sulfonic acid (ANS) in aqueous dispersions of dioleoylphosphatidylethanolamine (DOPE) and phosphatidylethanolamine transphosphatidylated from egg phosphatidylcholine (TPE) was measured. The orientational order parameter and rotational diffusion constant of the lipophilic probe 1-(4-trimethylammoniumphenyl)-6-phenyl-1,3,5-hexatriene (TMA-DPH) were also determined in TPE dispersions. In agreement with a previous study on DOPE (Cheng (1989) Biophys. J. 55, 1025-1031), abrupt changes in both the order packing and rotational diffusion constant were found at the lamellar liquid crystalline (L alpha) to inverted hexagonal (HII) phase transition of TPE. Owing to the subnanosecond resolution capability of this frequency domain fluorometric technique, the heterogeneous fluorescence decay of ANS was resolved into three distinct components with different decay lifetimes (tau's). They were 0 less than tau less than 0.5 ns, 2 less than tau less than 9 ns and tau greater than 15 ns. These lifetime regions were attributed to the partitioning of ANS into the bulk aqueous medium, the lipid/water interface and the lipid hydrocarbon region, respectively. These classifications of lifetime regions were further supported by the sensitivity of those lifetime components with the solvent isotopic shift of D2O. Similar to the changes of orientational order and rotational diffusion of lipophilic probe, the lifetime and intensity fraction of ANS associated with the lipid/water interfacial region declined abruptly at the L alpha-HII transition of both DOPE and TPE. This observation suggested that a dehydration of the lipid headgroup surface occurs at the L alpha-HII transition. This study provided evidence that both the lipid headgroup surface hydration and the lipid dynamics change drastically as a result of the macroscopic rearrangement of lipids at the L alpha-HII transition.     

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.     

Time-resolved fluorescence of DAPI in solution and bound to polydeoxynucleotides

Fluorescence decay studies, obtained by multifrequency phase-modulation fluorometry, have been performed on DAPI in solution and complexed with natural and synthetic polydeoxynucleotides. DAPI decay at pH 7 was decomposed using two exponential components of 2.8 and 0.2 ns of lifetime values, respectively. The double exponential character of the decay was maintained over a large pH range. Phase- and modulation-resolved spectra, collected between 420 and 550 nm, have indicated at least two spectral components associated with the two lifetime values. This, plus the observation of the dependence of the emission spectrum on the excitation wavelength, suggests a lifetime heterogeneity originating from ground-state molecular conformers, partially affected by pH changes. DAPI complexed with natural polydeoxynucleotides retained most of the features of DAPI decay in solution, except for the value of the long lifetime component that was longer (approximately 4 ns) and the relative fractional fluorescence intensities of the two components that were inverted. AT polymers/DAPI complexes show single exponential decay. Solvent shielding when DAPI is bound to DNA changes the indole ring solvation and stabilizes the longer lifetime decay component. For poly(GC)/DAPI complex, the decay was similar to that of free DAPI in solution, proving the dependence on the polydeoxynucleotides sequence the different types of binding and the reliability of the fluorescence method to solve them.     

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)     

Tryptophan interactions of gramicidin A' channels in lipids: a time-resolved fluorescence study

The evolution of the incorporation of cation transport channels into lysolecithin micelles by gramicidin A was followed by measuring the ns time-resolved fluorescence of the tryptophan residues. In all samples, the tryptophan fluorescence could be resolved into three exponentially decaying components. The three decay times ranged from 6 to 8 ns, 1.8 to 3 ns, and 0.3 to 0.8 ns, depending on the emission wavelength. The fractional fluorescence of each component changed with incubation time. The long lifetime component had a reduced contribution to the total fluorescence while the short decay time component increased. The fluorescence spectra could be resolved into three distinct fluorescent components having maxima at 340 nm, 330 nm and 323 nm after 90 min of incubation, and 335 nm, 325 nm and 320 nm after 24 h of incubation. These maxima were, respectively, associated with the long, medium and short decay components. The fluorescence decay behaviour was interpreted as representing three families of tryptophans, the short lifetime component being due to a stacking interaction between tryptophan residues. The variation with incubation time suggests a two-step process in the channel-lipid organization. The first is associated with the conformational change of the polypeptide as it takes up a left-handed helical head-to-head dimer structure in the lipid. The second step is proposed to involve changes originating from membrane assembly and intermolecular interactions between channels as they form hexameric clusters.     

Pressure-induced perturbation of ANS-apomyoglobin complex: frequency domain fluorescence studies on native and acidic compact states.

The pressure dependence of the flexibility of the 8-anilino-1-naphthalene sulfonate (ANS)-apomyoglobin complex was investigated in the range between atmospheric pressure and 2.4 kbar by frequency domain fluorometry. We examined two structural states: native and acidic compact. The conformational dynamics of the ANS-apomyoglobin complex were deduced by studying the emission decay of ANS, which can form a noncovalent complex with the apoprotein in both the native and the acidic compact forms. Because the free fluorophore has a very short lifetime (less than 75 ps), its contribution can be separated from the long-lived emission. The latter arises from ANS molecules bound to the protein and provides information on the structural and dynamic characteristics of the macromolecule. The fluorescence emission decay of the ANS-apomyoglobin complex at neutral pH has a broad fluorescence lifetime distribution (width at half-maximum = 4.1 ns). The small changes in the fluorescence distribution parameters that occur with changes in pressure indicate that the ANS-apomyoglobin complex at neutral pH holds its compactness even at 2.4 kbar. A small contraction of molecular volume has been detected at low pressure, followed by a slight swelling with an increase in flexibility at higher pressures. The heterogeneity of ANS fluorescence in the acidic compact state of apomyoglobin is even greater than that in the native form (distribution width = 10 ns); moreover, the acidic compact state appears more expanded and accessible to solvent molecules than the native state, as suggested by the distribution center, which is 11 ns for the former and 19 ns for the latter. The lifetime distribution center remains constant with increasing pressure, which suggests that no other binding site is formed at high pressure.     

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)     

Time-resolved fluorescence studies of tryptophan mutants of Escherichia coli glutamine synthetase: conformational analysis of intermediates and transition-state complexes.

Single tryptophan-containing mutants of low adenylylation state Escherichia coli glutamine synthetase have been studied by frequency-domain fluorescence spectroscopy in the presence of various substrates and inhibitors. At pH 6.5, the Mn-bound wild-type enzyme (wild type has two tryptophans/subunit) and the mutant enzymes exhibit heterogeneous fluorescence decay kinetics; the individual tryptophans are adequately described by a triple exponential decay scheme. The recovered lifetime values are 5.9 ns, 2.6 ns, and 0.4 ns for Trp-57 and 5.8 ns, 2.3 ns, and 0.4 ns for Trp-158. These values are nearly identical to the previously reported results at pH 7.5 (Atkins, W.M., Stayton, P.S., & Villafranca, J.J., 1991, Biochemistry 30, 3406-3416). In addition, Trp-57 and Trp-158 both exhibit an ATP-induced increase in the relative fraction of the long lifetime component, whereas only Trp-57 is affected by this ligand at pH 7.5. The transition-state analogue L-methionine-(R,S)-sulfoximine (MSOX) causes a dramatic increase in the fractional intensity of the long lifetime component of Trp-158. This ligand has no effect on the W158S mutant protein and causes a small increase in the fractional intensity of the long lifetime component of the W158F mutant protein. Addition of glutamate to the ATP complex, which affords the gamma-glutamylphosphate-ADP complex, results in the presence of new lifetime components at 7, 3.2, and 0.5 ns for Trp-158, but has no effect on Trp-57. Similar results were obtained when ATP was added to the MSOX complex; Trp-57 exhibits heterogeneous fluorescence decay with lifetimes of 7, 3.5, and 0.8 ns. Decay kinetics of Trp-158 are best fit to a nearly homogeneous decay with a lifetime of 5.5 ns in the MSOX-ATP inactivated complex. These results provide a model for the sequence of structural and dynamic changes that take place at the Trp-57 loop and the central loop (Trp-158) during several intermediate stages of catalysis.     

Lipid domain structure correlated with membrane protein function in placental microvillus vesicles

Membrane fluidity properties of placental microvillus membrane vesicles (MVV) were determined from fluorescence anisotropy (r), dynamic depolarization, and lifetime heterogeneity studies of diphenylhexatriene (DPH), trimethylamino-DPH (TMA-DPH), and cis- and trans-parinaric acids (c-PnA and t-PnA). Plots of r against temperature for DPH and TMA-DPH in MVV had slope discontinuities at 26 degrees C (Tc, transition temperature); however, analysis of r in terms of probe rotational rate (R), limiting anisotropy (r infinity), and lifetime (tau) revealed that DPH reported a phase transition because of changes in r infinity, whereas the phase transition observed by TMA-DPH occurred primarily because of changes in R. Heterogeneity analysis using phase and modulation lifetimes at three frequencies showed that DPH and TMA-DPH lifetimes were homogeneous in MVV. Both long (greater than 25 ns) and short (less than 6 ns) lifetime components were detected for c-PnA and t-PnA in MVV, corresponding to the probes in solid and fluid lipid phases. The fractional amplitude of the long lifetimes (solid phase) decreased from 0.86 to 0.12 with increasing temperature (5-55 degrees C) as the membrane passed through the phase transition, with 50% of the change occurring at 27 degrees C (c-PnA) or 33 degrees C (t-PnA). The activation energies for alkaline phosphatase, aminopeptidase M, and sodium-proton antiporter activities all showed discontinuities in the temperature range 27-31 degrees C.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fluorescence lifetime distributions in proteins.

The fluorescence lifetime value of tryptophan residues varies by more than a factor of 100 in different proteins and is determined by several factors, which include solvent exposure and interactions with other elements of the protein matrix. Because of the variety of different elements that can alter the lifetime value and the sensitivity to the particular environment of the tryptophan residue, it is likely that non-unique lifetime values result in protein systems. The emission decay of most proteins can be satisfactorily described only using several exponential components. Here it is proposed that continuous lifetime distributions can better represent the observed decay. An approach based on protein dynamics is presented, which provides fluorescence lifetime distribution functions for single tryptophan residue proteins. First, lifetime distributions for proteins interconverting between two conformations, each characterized by a different lifetime value, are derived. The evolution of the lifetime values as a function of the interconversion rate is studied. In this case lifetime distributions can be obtained from a distribution of rates of interconversion between the two conformations. Second, the existence of a continuum of energy substates within a given conformation was considered. The occupation of a particular energy substate at a given temperature is proportional to the Boltzmann factor. The density of energy states of the potential well depends upon the width of the well, which determines the degree of freedom the residue can move in the conformational space. Lifetime distributions can be obtained by association of each energy substate with a different lifetime value and assuming that the average conformation can change as the energy of the substate is increased.(ABSTRACT TRUNCATED AT 250 WORDS)     

3-[p-(6-phenyl)-1,3,5-hexatrienyl]phenylpropionic acid (PA-DPH): characterization as a fluorescent membrane probe and binding to fatty acid binding proteins

The negatively charged fluorophore 3-[p-(6-phenyl)-1,3,5-hexatrienyl]phenylpropionic acid (PA-DPH) was characterized by comparison with its parent compound DPH, and with cationic trimethylammonium-DPH (TMA-DPH). The molar absorption coefficient of PA-DPH (60,000 cm-1.mol-1) as well as its quantum yield (0.7) and fluorescence lifetime (5 ns) in fluid phase membranes are intermediate between DPH and TMA-DPH. Steady-state fluorescence polarization studies show that PA-DPH detects the phase transition of both neutral and anionic bilayers. In fluid phase membranes the absolute values of PA-DPH polarization are considerably higher than DPH and somewhat lower than TMA-DPH. The results suggest that like TMA-DPH, PA-DPH is anchored to the surface of the membrane by its charge, but that it is probing a region somewhat deeper along the bilayer normal. PA-DPH binds to rat hepatic fatty acid binding protein (hFABP) and bovine serum albumin at PA-DPH/protein molar ratios of 1.5:1 and at least 6:1, respectively. Native oleic acid competes with PA-DPH for binding to both proteins, suggesting that the two ligands compete for similar binding sites. The affinity of PA-DPH for hFABP is similar to that of oleic acid. Thus, PA-DPH should be useful both as an anionic fluorescent membrane probe and a long-chain free fatty acid analogue.     

Fluorescence lifetime distributions of diphenylhexatriene-labeled phosphatidylcholine as a tool for the study of phospholipid-cholesterol interactions.

Fluorescence lifetimes of 1-palmitoyl-2-diphenylhexatrienylpro-pionyl-phosphatidylc hol ine in vesicles of palmitoyloleoyl phosphatidylcholine (POPC) (1:300, mol/mol) in the liquid crystalline state were determined by multifrequency phase fluorometry. On the basis of statistic criteria (chi 2red) the measured phase angles and demodulation factors were equally well fitted to unimodal Lorentzian, Gaussian, or uniform lifetime distributions. No improvement in chi 2red could be observed if the experimental data were fitted to bimodal Lorentzian distributions or a double exponential decay. The unimodal Lorentzian lifetime distribution was characterized by a lifetime center of 6.87 ns and a full width at half maximum of 0.57 ns. Increasing amounts of cholesterol in the phospholipid vesicles (0-50 mol% relative to POPC) led to a slight increase of the lifetime center (7.58 ns at 50 mol% sterol) and reduced significantly the distributional width (0.14 ns at 50 mol% sterol). Lifetime distributions of POPC-cholesterol mixtures containing greater than 20 mol% sterol were within the resolution limit and could not be distinguished from monoexponential decays on the basis of chi 2red. Cholesterol stabilizes and rigidifies phospholipid bilayers in the fluid state. Considering its effect on lifetime distributions of fluorescent phospholipids it may also act as a membrane homogenizer.     

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.     

Frequency domain measurements of the fluorescence lifetime of ribonuclease T1.

Using multifrequency phase/modulation fluorometry, we have studied the fluorescence decay of the single tryptophan residue of ribonuclease T1 (RNase T1). At neutral pH (7.4) we find that the decay is a double exponential (tau 1 = 3.74 ns, tau 2 = 1.06 ns, f1 = 0.945), in agreement with results from pulsed fluorometry. At pH 5.5 the decay is well described by a single decay time (tau = 3.8 ns). Alternatively, we have fitted the frequency domain data by a distribution of lifetimes. Temperature dependence studies were performed. If analyzed via a double exponential model, the activation energy for the inverse of the short lifetime component (at pH 7.4) is found to be 3.6 kcal/mol, as compared with a value of 1.0 kcal/mol for the activation energy of the inverse of the long lifetime component. If analyzed via the distribution model, the width of the distribution is found to increase at higher temperature. We have also repeated, using lifetime measurements, the temperature dependence of the acrylamide quenching of the fluorescence of RNase T1 at pH 5.5. We find an activation energy of 8 kcal/mol for acrylamide quenching, in agreement with our earlier report.     

Conformational dynamics of bovine Cu, Zn superoxide dismutase revealed by time-resolved fluorescence spectroscopy of the single tyrosine residue.

The structural dynamics of bovine erythrocyte Cu, Zn superoxide dismutase (BSOD) was studied by time-resolved fluorescence spectroscopy. BSOD is a homodimer containing a single tyrosine residue (and no tryptophan) per subunit. Frequency-domain fluorometry revealed a heterogeneous fluorescence decay that could be described with a Lorentzian distribution of lifetimes. The lifetime distribution parameters (center and width) were markedly dependent on temperature. The distribution center (average lifetime) displayed Arrhenius behavior with an Ea of 4.2 kcal/mol, in contrast with an Ea of 7.4 kcal/mol for the single-exponential decay of L-tyrosine. This indicated that thermal quenching of tyrosine emission was not solely responsible for the effect of temperature on the lifetimes of BSOD. The distribution width was broad (1 ns at 8 degrees C) and decreased significantly at higher temperatures. Furthermore, the width of the lifetime distribution increased in parallel to increasing viscosity of the medium. The combined effects of temperature and viscosity on the fluorescence decay suggest the existence of multiple conformational substrates in BSOD that interconvert during the excited-state lifetime. Denaturation of BSOD by guanidine hydrochloride produced an increase in the lifetime distribution width, indicating a larger number of conformations probed by the tyrosine residue in the denatured state. The rotational mobility of the tyrosine in BSOD was also investigated. Analysis of fluorescence anisotropy decay data enabled resolution of two rotational correlation times. One correlation time corresponded to a fast (picosecond) rotation that contributed 62% of the anisotropy decay and likely reported local mobility of the tyrosine ring. The longer correlation time was 50% of the expected value for rotation of the whole (dimeric) BSOD molecule and appeared to reflect segmental motions in the protein in addition to overall tumbling. Comparison between rotational correlation times and fluorescence lifetimes of BSOD indicates that the heterogeneity in lifetimes does not arise from mobility of the tyrosine per se, but rather from dynamics of the protein matrix surrounding this residue which affect its fluorescence decay.