Time-resolved FRET fluorescence spectroscopy of visible fluorescent protein pairs.

Förster resonance energy transfer (FRET) is a powerful method for obtaining information about small-scale lengths between biomacromolecules. Visible fluorescent proteins (VFPs) are widely used as spectrally different FRET pairs, where one VFP acts as a donor and another VFP as an acceptor. The VFPs are usually fused to the proteins of interest, and this fusion product is genetically encoded in cells. FRET between VFPs can be determined by analysis of either the fluorescence decay properties of the donor molecule or the rise time of acceptor fluorescence. Time-resolved fluorescence spectroscopy is the technique of choice to perform these measurements. FRET can be measured not only in solution, but also in living cells by the technique of fluorescence lifetime imaging microscopy (FLIM), where fluorescence lifetimes are determined with the spatial resolution of an optical microscope. Here we focus attention on time-resolved fluorescence spectroscopy of purified, selected VFPs (both single VFPs and FRET pairs of VFPs) in cuvette-type experiments. For quantitative interpretation of FRET-FLIM experiments in cellular systems, details of the molecular fluorescence are needed that can be obtained from experiments with isolated VFPs. For analysis of the time-resolved fluorescence experiments of VFPs, we have utilised the maximum entropy method procedure to obtain a distribution of fluorescence lifetimes. Distributed lifetime patterns turn out to have diagnostic value, for instance, in observing populations of VFP pairs that are FRET-inactive.

Pulse fluorimetry study of energy transfers between tryptophan residues and NADPH in beef liver glutamate dehydrogenase complexes.

A method is proposed to determine the rates of singlet energy transfers in an array of chromophores containing a finite number of donors and fluorescent acceptors. This method is based on measurements of transfer efficiency coupled with pulse fluorimetry. Three classes of donors can be distinguished which differ in their energy transfer rate. The rates of the first, the second and the third class are respectively greater than, of the order of, and smaller than the emission rate. The method is applied to the study of the energy transfers from tryptophan residues to NADPH, in ternary and quaternary glutamate dehydrogenase complexes. Practically, all these tryptophan residues belong to the first class. They can be divided into two subclasses having different transfer rate values. The distance between these residues and the NADPH site are of the order of 2.5 nm. In addition, the ligand binding induces a protein conformation change, leading to a fluorescence quenching of the tryptophanyl emission.

Structural investigations of basic amphipathic model peptides in the presence of lipid vesicles studied by circular dichroism, fluorescence, monolayer and modeling.

A cationic amphiphilic peptide made of 10 leucine and 10 lysine residues, and four of its fluorescent derivatives in which leucines were substituted by Trp residues at different locations on the primary sequence have been synthesized. The interactions of these five peptides with neutral anionic or cationic vesicles were investigated using circular dichroism, steady state and time-resolved fluorescence with a combination of Trp quenching by brominated lipid probes, monolayers, modeling with minimization and simulated annealing procedures. We show that all the five peptides interact with neutral and anionic DMPC, DMPG, DOPC or egg yolk PC vesicles. The binding takes place whatever the peptide conformation in solution is. In the case of DMPC bilayers the binding free energy DeltaG is estimated at -8 kcal mole-1 and the number of phospholipid molecules involved is about 20-25 per peptide molecule. Peptides are bound as single-stranded alpha helices orientated parallel to the bilayer surface. In the anchoring of phospholipid head groups around the peptides, the lipid molecules are not smeared out in a plane parallel to the membrane surface but are organized around the hydrophilic face of the alpha helices like 'wheat grains around an ear' and protrude outside the bilayer towards the solvent. We suggest that such a lipid arrangement generates transient structural defects responsible for the membrane permeability enhancement. When an electrical potential is applied, the axis of the peptide helices remains parallel to the membrane surface and does not reorient to give rise to a bundle of helix monomers that forms transmembrane channels via a 'barrel stave' mechanism. The penetration depth of alpha helices in relation to the position of phosphorus atoms in the unperturbed lipid leaflet is estimated at 3.2 A.

An experimental study of the electronic absorption and fluorescence spectral properties of new p-substituted-N-phenylpyrroles and their electrosynthesized polymers.

Electronic absorption and fluorescence spectral properties of new p-substituted-N-phenylpyrroles (N-PhPys), including HOPhPy, MeOPhPy, ThPhPy, PhDPy, DPhDPy, PyPhThThPhPy, and their available, electrosynthesized polymers were investigated. Electronic absorption spectra, fluorescence excitation and emission spectra, fluorescence quantum yields (ΦF) and lifetimes (τF), and other photophysical parameters of these N-PhPy derivatives and their polymers were measured in DMF, DMSO diluted solutions and/or solid state at room temperature. The electronic absorption spectra of N-PhPy derivatives and their polymers included one to several bands, located in the 270-395 nm region, according to the p-phenyl substituent electron-donating effect and conjugated heteroaromatic system length. The fluorescence excitation spectra were characterized by one broad main peak, with, in most cases, one (or more) poorly resolved shoulder (s), appearing in the 270-405 nm region, and their emission spectra were generally constituted of several bands located in the 330-480 nm region. No significant shift of the absorption, fluorescence excitation and emission spectra wavelengths was found upon going from the monomers to the corresponding polymers. ΦF values were high, varying between 0.11 and 0.63, according to the nature of substituents(s) and to the conjugated system extension. Fluorescence decays were mono-exponential for the monomers and poly-exponential for PyPhThThPhPy and for polymers. τF values were relatively short (0.35-5.17 ns), and markedly decreased with the electron-donor character of the phenyl group p-substituent and the conjugated system extension.

A new method for decay-associated fluorescence spectroscopy. Application to the tryptophan zwitterion.

We describe a new method for decay associated fluorescence spectroscopy using synchrotron radiation as the excitation pulse and a photon counting technique. This method is based on the determination of the difference between the barycenters of the exciting pulse and of the fluorescence response at several wavelengths. It is applicable to the case where individual decay times are independent of emission wavelength. Coupled to the analysis of the decay curve at only one emission wavelength, this method reduces the time devoted to the numerical analysis and avoids the spectral distortion due to the lamp profile. The results obtained by this method on indole, the tryptophan zwitterion, and N-acetyl-tryptophan are presented. Results are compared to those obtained by two other methods: Determination of the fluorescence decay parameters by deconvolution analysis at several emission wavelengths. Photon counting of the fluorescence spectrum emitted during a selected time window after the excitation pulse.

[Intensity and anisotropy decays measurement of perylene in pigeon erythrocyte membrane. Comparison with an isotropic viscous medium (author's transl)]. / Mesure des déclins de l'intensité et de l'anisotropie de fluorescence du pérylène en Présence de membranes d'érythrocyte de pigeon. Comparaison avec un milieu isotrope visqueux.

Using synchrotron radiation as the excitation light, we studied the fluorescence parameters of perylene incubated with pigeon erythrocyte membranes and with an isotropic viscous medium, the Primol 342 oil. From 4 to 37 degrees C, we observed a single lifetime of 4.5 ns in the oil and two with the membrane (tau 1 = 1-1.4 ns and tau 2 = 5.4-6.1 ns). The dependence upon temperature of the rotation correlation time of perylene (theta) in the oil was characteristic of an isotropic medium, whereas the limiting value of anitropy (r infinity) was zero. With the membrane, r infinity decreased from 0.14 to 0.06 and theta from 2.9 to 0.5 ns, indicating a greater amplitude and frequency of molecular motions. The addition of chlorpromazine, indomethacine, tetracaine, n-octylamine, octanol or octanoic acid to the membrane decreased the tau 1 and tau 2 values. This would stem from the disorganization of the membrane induced by the drugs.

[Interactions of HIV-1 DNA heterocyclic bases with viral DNA]. / Izuchenie vzaimodeistvii geterotsiklicheskikh osnovanii DNK VICH-1 s virusnoi integrazoi.

Human immunodeficiency virus type 1 integrase is one of three viral enzymes, and it realizes a key process of the viral replication cycle, i.e. viral DNA integration into infected cell genome. Integrase recognizes nucleotide sequences located at the ends of the viral DNA U3 and U5 LTRs and catalyzes 3'-processing and strand transfer reactions. To study the interactions between integrase and viral DNA at present work, we used modified integrase substrates mimicking the terminal U5 LTR sequence and containing non-nucleoside insertions in one or/and both strands. It is shown that the substrate modifications have no influence on the integrase binding rate, while the heterocyclic bases removal in the 5th and 6th substrate positions and in the 3rd position of the substrate processed strand distinctly inhibits the integrase catalytic activity. This fact demonstrates these bases significance for the active enzyme/substrate complex formation. On the contrary, modification of the 3rd position within substrate non-processed strand stimulates 3'-processing. Since heterocyclic base elimination results in disruption of the DNA complementary and staking interactions, this result shows that DNA double helix destabilization close to the cleaved bond promotes the 3'-processing.

Analyzing the distribution of decay constants in pulse-fluorimetry using the maximum entropy method.

The maximum entropy method (MEM) is used to analyze time-resolved pulse-fluorescence spectrometry. The central problem in such analyses is the recovery of the distribution of exponentials describing the decay of the fluorescence (i.e., inverting the Laplace transform) which is, in turn, convolved by the shape of the excitation flash. MEM is shown to give high quality results from both computer-generated "noisy" data and experimental data from chemical and biological molecules.The use of the Shannon-Jaynes entropy function is justified and both the theoretical and practical advantages of MEM are presented. The MEM results are easy to interpret and can help to overcome some experimental limitations. In particular MEM could be a powerful tool to analyze the heterogeneity of fluorescent emission of biological macromolecules which can be correlated with their conformational dynamics in solution.

Pressure effects on the physical properties of lipid bilayers detected by trans-parinaric acid fluorescence decay.

The effects of hydrostatic pressure on the physical properties of large unilamellar vesicles of single lipids dipalmitoyl phosphatidylcholine (DPPC) and dimyristoyl phosphatidylcholine (DMPC) and lipid mixtures of DMPC/DPPC have been studied from time-resolved fluorescence of trans-parinaric acid. Additional experiments were carried out using diphenylhexatriene to compare the results extracted from both probes. Fluorescence decays were analyzed by the maximum entropy method. Pressure does not influence the fluorescence lifetime distribution of trans-parinaric acid in isotropic solvents. However, in pressurized lipid bilayers an abrupt change was observed in the lifetime distribution which was associated with the isothermal pressure-induced phase transition. The pressure to temperature equivalence values, dT/dP, determined from the midpoint of the phase transitions, were 24 and 14.5 degrees C kbar-1 for DMPC and POPC, respectively. Relatively moderate pressures of about 500 bar shifted the DMPC/DPPC phase diagram 11.5 degrees C to higher temperatures. The effects of pressure on the structural properties of these lipid vesicles were investigated from the anisotropy decays of both probes. Order parameters for all systems increased with pressure. In the gel phase of POPC the order parameter was smaller than that obtained in the same phase of saturated phospholipids, suggesting that an efficient packing of the POPC hydrocarbon chains is hindered.

Picosecond tryptophan fluorescence of thioredoxin: evidence for discrete species in slow exchange.

The steady-state tryptophan fluorescence and time-resolved tryptophan fluorescence of Escherichia coli thioredoxin, calf thymus thioredoxin, and yeast thioredoxin have been studied. In all proteins, the tryptophan residues undergo strong static and dynamic quenching, probably due to charge-transfer interactions with the nearby sulfur atoms of the active cysteines. The use of a high-resolution photon counting instrument, with a time response of 60 ps full width at half-maximum, allowed the detection of fluorescence lifetimes ranging from a few tens of picoseconds to 10 ns. The data were analyzed both by classical nonlinear least squares and by a new method of entropy maximization (MEM) for the recovery of lifetime distributions. Simulations representative of the experimental data were used to test the MEM analysis. Strong support was obtained in this way for a small number of averaged discrete species in the fluorescence decays. Wavelength studies show that each of these components spreads over closely spaced excited states, while the temperature studies indicate that they do not exchange significantly on the nanosecond time scale. The oxidized form of thioredoxin is characterized by a high content of a very short lifetime below 70 ps, the amplitude of which is sharply decreased upon reduction. On the other hand, the fluorescence anisotropy decays indicate that reduction causes an increase of the very fast tryptophan rotations in an otherwise relatively rigid structure. While the calf thymus and E. coli proteins have mostly similar dynamical fluorescence properties, the yeast thioredoxin differs in many respects.

Conformational fluctuations and protein reactivity. Determination of the rate-constant spectrum and consequences in elementary biochemical processes.

When a protein's active site happens to be strongly coupled with the protein structure, the rate constant of the reaction may eventually be modulated by the conformational fluctuations. Evidence for this effect has long been provided by extensive flash photolysis investigations of liganded hemoproteins and more recently of the non-heme respiratory protein hemerythrin in hydro-organic solvents. Within a given protein conformational substate, an elementary reaction step is characterized by one single free energy barrier and by a first-order rate constant, k, which changes with temperature according to an Arrhenius law. At physiological temperature and low viscosity, ultrafast conformational relaxation causes efficient averaging of the reaction rates and the protein displays exponential kinetics with an average rate constant (k). Under sufficiently general conditions, it can be shown that (k) also follows a simple Arrhenius law with 'effective' values of the pre-exponential factor Aeff and activation enthalpy Heff. It is found that Aeff strongly depends on the overall shape of the rate constant distribution and that Heff actually corresponds to the lower limit of the enthalpy of activation, i.e. the value associated with the highest possible reaction rate. The underlying distribution of rate constants can be reconstructed from a set of experiments in which the kinetics depart from an exponential, i.e. at low temperature and high viscosity. The most probable distribution of exponentials consistent with the observed kinetics of the geminate recombinations of oxygen with photodissociated hemerythrin has been determined by using a new approach, known as the maximum entropy method. The results are consistent with a single pre-exponential value and a distributed enthalpy spectrum. As expected, Heff does not coincide either with the most probable nor with the average value of the enthalpy. The most salient findings are that the probability for any protein molecule to have an enthalpy of activation equal to the effective value Heff vanishes and that Aeff differs by nearly three orders of magnitude from the true value A0. Biochemical reaction rates are actually average values, since protein reactions are measured under physiological conditions, where conformational relaxation is always fast. Our understanding of the significance of Aeff and Heff is therefore entirely dependent on the knowledge of the distribution function of the rate constants. In particular, enthalpy and entropy terms of similar reactions performed by different proteins cannot be compared as long as the distribution of the rate constants remains unknown.

Pressure effects on the lateral distribution of cholesterol in lipid bilayers: a time-resolved spectroscopy study.

The effects of hydrostatic pressure and temperature on the phase behavior and physical properties of the binary mixture palmitoyloleoylphosphatidylcholine/cholesterol, over the 0-40 molar % range of cholesterol compositions, were determined from the changes in the fluorescence lifetime distribution and anisotropy decay parameters of the natural lipid trans-parinaric acid (t-PnA). Pressurized samples were excited with a Ti-sapphire subpicosecond laser, and fluorescence decays were analyzed by the quantified maximum entropy method. Above the transition temperature (T(T) = -5 degrees C), at atmospheric pressure, two liquid-crystalline phases, alpha and beta, are formed in this system. At each temperature and cholesterol concentration below the transition pressure, the fluorescence lifetime distribution pattern of t-PnA was clearly modulated by the pressure changes. Pressure increased the fraction of the liquid-ordered beta-phase and its order parameter, but it decreased the amount of cholesterol in this phase. Palmitoyloleoylphosphatidylcholine/cholesterol phase diagrams were also determined as a function of temperature and hydrostatic pressure.

Liquid-crystalline phases of cholesterol/lipid bilayers as revealed by the fluorescence of trans-parinaric acid.

The presence of two liquid-crystalline phases, alpha and beta, in mixed bilayers of dimyristoylphosphatidylcholine/cholesterol was detected by the changes in the distribution of the fluorescence lifetimes of t-PnA, as analyzed by the Maximum Entropy Method. The formation of the liquid-ordered beta-phase, in the 30-40 degrees C temperature range as a function of cholesterol concentration (0-40 mol%), could be related quantitatively to the relative amplitude of a long lifetime component of the probe (10-14 ns). Based on this evidence, the phase behavior of mixtures of the unsaturated lipid palmitoyloleoylphosphatidylcholine and cholesterol was determined using the same technique, for cholesterol concentrations in the 0-50 mol% range, between 10 and 40 degrees C. It was found that two liquid-crystalline phases are also formed in this system, with physical properties reminiscent of the alpha- and beta-phases formed with saturated lipids. However, in this case it was determined that, for temperatures in the physiological range, the alpha- and beta-phases coexist up to 40 mol% cholesterol. This finding may be of significant biological relevance, because it supports the long held notion that cholesterol is responsible for the lipid packing heterogeneity of several natural membranes rich in unsaturated lipid components.

Recovery of lifetime distributions from frequency-domain fluorometry data by means of the quantified maximum entropy method.

The new quantified version of the maximum entropy method allows one to recover lifetime distributions with a precise statement of the accuracy of position, surface, and broadness of peaks in the distribution. Applications to real data (2,6-ANS in aqueous solutions of sodium dodecyl sulfate micelles of Β-cyclodextrin) are presented.

Nanosecond dynamics of horse heart apocytochrome c in aqueous solution as studied by time-resolved fluorescence of the single tryptophan residue (Trp-59).

The time-resolved fluorescence emission characteristics of the single tryptophan residue (Trp-59) of horse heart apocytochrome c--the precursor of the intramitochondrial cytochrome c--were studied in aqueous solution. The total fluorescence intensity decay measured over the whole emission spectrum was analyzed as a sum of three or four exponentials by the nonlinear least-squares method, the last model always providing a slight but significant decrease in the chi 2 values. Maximum entropy analysis, recently developed for time-resolved fluorometry (Livesey et al., 1987; Livesey & Brochon, 1987), strongly suggests the existence of a distribution including at least four separate classes of lifetimes. The center values were around 0.1-0.2, 1, 3, and 5 ns, in agreement with the lifetime values obtained by nonlinear least-squares regression analysis. As a function of the emission wavelength, these values remained constant within the experimental error, whereas a redistribution of the fractional amplitudes was observed: the contributions of the short components increased in the blue edge region of the emission spectrum. Temperature increase led essentially to a redistribution of the fractional amplitudes, affecting mostly that of the 5-ns component, which almost totally disappeared at high temperature (35-40 degrees C). The lifetime values were not significantly affected except for the 3-ns component, which decreased by about 15% in the temperature range studied. Such observations strongly suggest that the protein exists under different conformational substates in thermal equilibrium. Time-resolved fluorescence anisotropy measurements evidenced the existence of fast internal rotation of the Trp residue. An average maximum restricted angle of rotation of around 55 degrees was calculated. A second internal motion, slower by 1 order of magnitude, corresponding likely to a local motion of the peptide chain involving the Trp-59 residue, was detected on the anisotropy decay curve. Finally, the longest correlation time (5 ns) should correspond to the average rotation of the overall protein. Its value doubled as a function of the protein concentration, revealing an association process leading most likely to a dimer in the concentration range studied (2-139 microM). The flexibility of the peptide chain was more restrained in the associated than in the monomeric form, but the fast internal rotation of the Trp residue was not.

Lipid clustering in bilayers detected by the fluorescence kinetics and anisotropy of trans-parinaric acid.

Fluid heterogeneity in lipid bilayers and shows a simple and useful method to quantify this heterogeneity. Taking advantage of the maximum entropy method, we have resolved the probe fluorescence lifetime distributions in homogeneous solutions and in single and two-component lipid bilayers at different temperatures. A precise description of the emission kinetics was obtained as a function of viscosity in the homogeneous solution and as a function of the phase composition (gel/fluid) in the lipid bilayers. These data show, unambiguously, that the same distribution pattern, with two well resolved lifetime classes, is observed both in pure solvents and in fluid bilayers. This distribution is modified during the thermotropic phase transition, with the appearance of a long lifetime component. The anisotropy experiments confirm that the amplitude of this component is proportional to the fraction of probe located in the gel phase. From this fraction we have quantified the amount of gel phase in the binary bilayer system dimyristoyl phosphatidylcholine/dipalmitoyl phosphatidylcholine and determined the thermotropic phase diagram of the mixture. This phase diagram agrees well with that calculated assuming ideal mixing of the lipids (Marbrey, S., and J.M. Sturtevant. 1976. Proc. Natl. Acad. Sci. USA. 73:862-3866).

Dynamics of the active loop of snake toxins as probed by time-resolved polarized tryptophan fluorescence.

The local environment and dynamics of the single tryptophan residue in the respective active loops of cardiotoxin and alpha-neurotoxin from Naja nigricollis and of erabutoxin b from Laticauda semifasciata have been studied by steady-state and time-resolved polarized fluorescence and analyzed with distributions of decay times. Trp11 in loop I of cardiotoxin exhibits a very broad and complex distribution of fluorescence lifetimes at 20 degrees C. Despite its relatively external location in the toxin, the residue appears to be partly shielded from water and shows restricted but significant conformational fluctuations on the picosecond and nanosecond time scales. The thermal stability of cardiotoxin allowed a study of its static and dynamic fluorescence properties over a large range of temperatures. Interconversions in the intermediate nanosecond range lead to a thorough reorganization of the cardiotoxin fluorescence lifetime distribution with temperature. On the contrary, the fluorescence kinetics of Trp29 in loop II of the two neurotoxins is dominated by about 80% of a major decay time, which suggests that a nearly unique local conformation of the toxin is maintained over all time scales above the sub-nanosecond range. The fluorescence anisotropy decays show that the residue also has extremely limited rotational freedom down to the picosecond time scale. These findings are in good agreement with structural and dynamic information previously reported on the different toxins from NMR and X-ray crystallographic studies. The different dynamic properties around the tryptophan residue of the cardiotoxin and neurotoxin active loops can be analyzed within the frame of their different respective mechanisms of toxicity.

Quenching by acrylamide and temperature of a fluorescent probe attached to the active site of ribonuclease.

The fluorescence properties of ribonuclease labelled at its active site with N-(iodoacetylamino)-ethyl-5-naphthylamine-1-sulfonic acid have been studied at different temperatures and in the presence of acrylamide. The rate constant for the quenching of the fluorescence of labelled ribonuclease by acrylamide is apparently not limited by the "accessibility" of the probe: similar values are obtained for the native and denatured states of the protein. Instead, acrylamide seems to be a rather inefficient quencher of this fluorescent group [acetamidoamino)ethyl-5-naphthylamine-1-sulfonic acid), as shown by non-linear Stern-Volmer representations, biphasic decay kinetics, and a low value of the rate constant. The fluorescence intensity of the native state of the labelled protein is highly sensitive to temperature and exhibits a 20% decrease for an increase of temperature of from 10 degrees C to 30 degrees C, independent of solvent viscosity. This thermal quenching is specific for the native conformation and disappears when the protein is unfolded. When the fluorescence lifetime of the label is shortened by addition of acrylamide, the effect of temperature becomes identical for native and unfolded structures. This suggests that the cause of the thermal quenching is the presence of conformational fluctuations within the native protein which apparently take place in the time range from 35 to 200 ns.