Spectral properties and function of two lumazine proteins from Photobacterium

The spectral properties are compared for two 6,7-dimethyl-8-ribityllumazine proteins from marine bioluminescent bacteria, one from a psychrophile, Photobacterium phosphoreum, and the other from a thermophile, Photobacterium leiognathi. The visible spectral properties, which are the ones by which the protein performs its biological function of bioluminescence emission, are almost the same for the two proteins: at 2 degrees C and 50 mM Pi, pH 7, fluorescence quantum yield phi F = 0.59 and 0.54, respectively; fluorescence lifetime tau = 14.4 and 14.8 ns, respectively; fluorescence maxima, both 475 nm; absorption maximum, 417 and 420 nm, respectively; circular dichroism minima at around 420 nm, both -41 X 10(3) deg cm2 dmol-1. The ligand binding sites therefore must provide very similar environments, and arguments are presented that the bound ligand is relatively exposed to solvent. The dissociation equilibrium was studied by steady-state fluorescence polarization. The thermophilic protein binds the ligand with Kd (20 degrees C) = 0.016 microM, 10 times more tightly than the other protein [Kd (20 degrees C) = 0.16 microM]. The origin of the binding difference probably resides in differences in secondary structure. The tryptophan fluorescence spectra of the two proteins are different, but more significant is an observation of the decay of the tryptophan emission anisotropy. For the psychrophilic lumazine protein this anisotropy decays to zero in 1 ns, implying that its single tryptophan residue lies in a very "floppy" region of the protein. For the other protein, the anisotropy exhibits both a fast component and a slow one corresponding to rotation of the protein as a whole.(ABSTRACT TRUNCATED AT 250 WORDS)     

Determination of rotational correlation times from deconvoluted fluorescence anisotropy decay curves. Demonstration with 6,7-dimethyl-8-ribityllumazine and lumazine protein from Photobacterium leiognathi as fluorescent indicators

The experimental and analytical protocols required for obtaining rotational correlation times of biological macromolecules from fluorescence anisotropy decay measurements are described. As an example, the lumazine protein from Photobacterium leiognathi was used. This stable protein (Mr 21 200) contains the noncovalently bound, natural fluorescent marker 6,7-dimethyl-8-ribityllumazine, which has in the bound state a long fluorescence lifetime (tau = 14 ns). Shortening of the fluorescence lifetime to 2.6 ns at room temperature was achieved by addition of the collisional fluorescence quencher potassium iodide. The shortening of tau had virtually no effect on the rotational correlation time of the lumazine protein (phi = 9.4 ns, 19 degrees C). The ability to measure biexponential anisotropy decay was tested by the addition of Photobacterium luciferase (Mr 80 000), which forms an equilibrium complex with lumazine protein. Under the experimental conditions used (2 degrees C) the biexponential anisotropy decay can best be described with correlation times of 20 and 60 ns, representing the uncomplexed and luciferase-associated lumazine proteins, respectively. The unbound 6,7-dimethyl-8-ribityllumazine itself (tau = 9 ns) was used as a model compound for determining correlation times in the picosecond time range. In the latter case rigorous deconvolution from the excitation profile was required to recover the correlation time, which was shorter (100-200 ps) than the measured laser excitation pulse width (500 ps).     

Spectroscopic investigations of the single tryptophan residue and of riboflavin and 7-oxolumazine bound to lumazine apoprotein from Photobacterium leiognathi

Spectroscopic techniques have been applied to investigate the conformation, local structure, and dynamic properties of the apoprotein of the lumazine protein from Photobacterium leiognathi and the holoprotein reconstituted with either the natural ligand 6,7-dimethyl-8-ribityllumazine or the closely related analogues riboflavin and 6-methyl-7-oxo-8-ribityllumazine (7-oxolumazine). The analogues are bound similarly to the natural prosthetic group. They exhibit similar shifts on binding in their absorption and fluorescence spectra, single-exponential fluorescence decays, and no independent motion from the protein as evident from a long-lived anisotropy decay (single-exponential phi = 10 ns, 20 degrees C) and high initial anisotropy. Steady-state anisotropy measurements result in similar KD's (40 nM, 20 degrees C, 50 mM inorganic phosphate) for all ligands. Circular dichroism in the far-UV region (190-250 nm) indicates no change in secondary structure on binding to the apoprotein. In the spectral region of 250-310 nm relatively large changes occur, indicating changes in the environment of the tyrosine and tryptophan residues. The single tryptophan residue shows a three-exponential decay of its fluorescence in both the apoprotein and the holoprotein. Radiationless energy transfer also occurs from the tryptophan to the bound ligand, especially evident with 7-oxolumazine. We have designed a new method for evaluation of the rate constant of energy transfer by measuring the (picosecond) rise time of the acceptor fluorescence. The anisotropy decay of the tryptophan residue shows two correlation times, a short one (phi approximately equal to 0.4 ns) representing rapid but restriced oscillation of this residue and a longer one (phi 2 = 5-7 ns, 20 degrees C) representing the motion of a larger segment of the protein.     

Electronic excitation transfer in the complex of lumazine protein with bacterial bioluminescence intermediates

Fluorescence dynamics measurements have been made on the bioluminescence reaction intermediates using Photobacterium leiognathi, Vibrio fischeri, and Vibrio harveyi luciferases, both alone and in mixtures with Photobacterium phosphoreum lumazine protein. Each luciferase produces a "fluorescent transient" intermediate on reaction with the bioluminescence substrates, FMNH2, tetradecanal, and O2, and all have a fluorescence quantum yield about 0.3, with a predominant lifetime around 10 ns. The P. leiognathi luciferase fluorescent transient has a rotational correlation time of 79 ns at 2 degrees C, as expected for the rotational diffusion of a 77-kDa macromolecule. In the presence of lumazine protein however a faster correlation time of about 3 ns predominates. This rapid channel of anisotropy loss is attributed to energy transfer from the flavin intermediate bound on the luciferase to the lumazine ligand, reflects the presence of protein-protein complexation, and is greatest in the case of P. leiognathi, but not at all for V. fischeri. This fact is consistent with the strong influence of lumazine protein on the bioluminescence reaction of P. leiognathi, and not at all with V. fischeri. The rate of energy transfer is of order 10(9) s-1, much greater than the 10(8) s-1 fluorescence rate of the donor. Thus the bioluminescence excitation of lumazine protein could occur by a similar photophysical mechanism of interprotein energy transfer from a chemically excited fluorescent transient donor to the lumazine acceptor.     

Bioluminescence spectral and fluorescence dynamics study of the interaction of lumazine protein with the intermediates of bacterial luciferase bioluminescence

The mechanism of the shifting of the bioluminescence spectrum from the reaction of bacterial luciferase by lumazine protein is investigated by methods of fluorescence dynamics. A metastable intermediate is produced on reaction of Vibrio harveyi luciferase with FMNH2 and O2. It has an absorption maximum at 374 nm and a rotational correlation time (phi) derived from the decay of its fluorescence (maximum 500 nm) anisotropy of 90 ns (2 degrees C). Lumazine protein from Photobacterium phosphoreum has an absorption maximum at 417 nm and a fluorescence maximum at 475 nm. Lumazine protein forms a protein-protein complex with luciferase, and the complex has a phi of approximately 100 ns. A mixture of lumazine protein and the intermediate would be expected to have an average correlation time (phi av) around 100 ns, but instead, the result is anomalous. The phi av is much lower and is also wavelength dependent. For excitation at 375 nm, which is mainly absorbed in the flavin chromophore of the intermediate, phi av = 25 ns, but at 415 nm, mainly absorbed by the lumazine derivative ligand of lumazine protein, phi av approximately 50 ns. It is proposed that protein-protein complexation occurs between lumazine protein and the luciferase intermediate and that in this complex energy transfer from the flavin to the lumazine is the predominant channel of anisotropy loss. A distance of 20 A between the donor and acceptor is calculated. In the bioluminescence reaction of intermediate with tetradecanal, a fluorescent transient species is produced which is the bioluminescence emitter.(ABSTRACT TRUNCATED AT 250 WORDS)     

Dynamics of supercoiled and linear pTZ18U plasmids observed with a long-lifetime metal-ligand complex

The metal-ligand complex, [Ru(bpy)2(dppz)]2+ (bpy = 2,2'-bipyridine, dppz = dipyrido[3,2-a:2',3'-c]phenazine) (Ru-BD), was used as a spectroscopic probe for studying nucleic acid dynamics. The Ru-BD complex displays a long lifetime of over 100 ns and a molecular light switch property upon DNA binding due to shielding of its dppz ligand from water. To further show the usefulness of this luminophore (Ru-BD) for probing DNA dynamics, we examined its intensity and anisotropy decays when intercalated into supercoiled and linear pTZ18U plasmids using frequency-domain fluorometry with a light-emitting diode (LED) as the modulated light source. Compared to the supercoiled plasmids with an average intensity decay time of 120.8 ns at 25 degrees C, we obtained somewhat longer lifetimes for the linear plasmids ((tau) = 141.4 ns at 25 degrees C), suggesting a more efficient shielding from water by the linear plasmids. The anisotropy decay data also showed longer rotational correlation times for the linear plasmids (495 and 35 ns at 25 degrees C) as compared to the supercoiled plasmids (412 and 27 ns at 25 degrees C). The slow and fast rotational correlation times appear to be consistent with the bending and torsional motions of the plasmids, respectively. The anisotropy values were quite similar, although the values of the supercoiled plasmids were slightly higher in both the steady-state and anisotropy decay measurements. These results indicate that Ru-BD can be applied in the study of both bending and torsional dynamics of nucleic acids.     

Nanosecond spectroscopy of retinol.

Nanosecond fluorescence spectroscopy was used to study the unique binding site of the retinol-binding protein (RBP) from human serum. At pH 7.4, the binding of retinol to RBP caused the following spectroscopic changes in the ligand: (a) an enhancement of the fluorescence decay time (gamma = 8 ns); and (b) an increase in the emission anisotropy (A = 0.29). Retinol in hexane has a fluorescent decay time of 4.2 ns and a low emission anisotropy (A = 0.02). The increase in the fluorescence decay time of bound retinol is not due to dielectric relaxation effects of polar groups, since nanosecond time-resolved emission spectra of either retinol in glycerol or retinol bound to RBP, failed to show any time-dependent shifts in emission maxima during the time period investigated 0 to 30 ns. The degree of rotational mobility of bound retinol was investigated by time emission anisotropy measurements. The observed rotational correlation time (theta = 7.2 ns) is consistent with a rigid compact macromolecule of 21,000 molecular weight.     

Dynamic fluorescence properties of bacterial luciferase intermediates

Three fluorescent species produced by the reaction of bacterial luciferase from Vibrio harveyi with its substrates have the same dynamic fluorescence properties, namely, a dominant fluorescence decay of lifetime of 10 ns and a rotational correlation time of 100 ns at 2 degrees C. These three species are the metastable intermediate formed with the two substrates FMNH2 and O2, both in its low-fluorescence form and in its high-fluorescence form following light irradiation, and the fluorescent transient formed on including the final substrate tetradecanal. For native luciferase, the rotational correlation time is 62 or 74 ns (2 degrees C) derived from the decay of the anisotropy of the intrinsic fluorescence at 340 nm or the fluorescence of bound 8-anilino-1-naphthalenesulfonic acid (470 nm), respectively. The steady-state anisotropy of the fluorescent intermediates is 0.34, and the fundamental anisotropy from a Perrin plot is 0.385. The high-fluorescence intermediate has a fluorescence maximum at 500 nm, and its emission spectrum is distinct from the bioluminescence spectrum. The fluorescence quantum yield is 0.3 but decreases on dilution with a quadratic dependence on protein concentration. This, and the large value of the rotational correlation time, would be explained by protein complex formation in the fluorescent intermediate states, but no increase in protein molecular weight is observed by gel filtration or ultracentrifugation. The results instead favor a proposal that, in these intermediate states, the luciferase undergoes a conformational change in which its axial ratio increases by 50%.     

Dynamic fluorescence study of the interaction of lumazine protein with bacterial luciferases

The equilibrium association of lumazine protein from Photobacterium phosphoreum with luciferases from either P. phosphoreum or an aldehyde-requiring dark mutant of Vibrio harveyi is measured from changes of the rotational correlation time which is derived from the decay of the lumazine ligand's fluorescence anisotropy. The rotational correlation time of lumazine protein is 23 ns (2 degrees C, 0.25 M Pi) and is increased on addition of luciferase due to the formation of a higher molecular weight complex. The V. harveyi luciferase exhibits full competence for the association and a 1:1 stoichiometry with a Kd in the range 40-90 microM. At lower ionic strength (0.05 M Pi), the Kd increases but is reduced again by the addition of dodecanol or dimyristoyllecithin. In contrast, tetradecanal, a substrate for the bioluminescence reaction, exerts no influence on the association. The equilibration rate is found to be too slow and for both luciferases the Kd values are too high for the interaction of the native proteins to account quantitatively for the spectral shifting of the bioluminescence by lumazine protein.     

Rapid relaxation processes in p-hydroxybenzoate hydroxylase from Pseudomonas fluorescens revealed by subnanosecond-resolved laser-induced fluorescence

Time-resolved fluorescence studies were carried out on the FAD bound to p-hydroxybenzoate hydroxylase from Pseudomonas fluorescens. The transient fluorescence exhibits complex decay kinetics with at least a short lifetime component in the 50-500-ps time region and a longer one in the range 1.5-3.5 ns. The shorter-lifetime component has a larger contribution in the presence of substrate (p-hydroxybenzoate) or inhibitor (p-aminobenzoate). The quenching of the fluorescence is both static and dynamic in nature. The decay of fluorescence anisotropy shows that the FAD environment is both flexible and rigid. The FAD mobility can be enhanced by dilution of the enzyme, by raising the temperature, or by the binding of substrate or inhibitors. The anisotropy results are interpreted in part in terms of a monomer-dimer equilibrium, whereby the FAD in the monomer contains much more flexibility. The above-mentioned effects induce a shift of the equilibrium to the monomeric side. From a constrained parameter fitting the dissociation constant is estimated to be about 1 microM for the free enzyme and somewhat higher for the binary complexes between the enzyme and substrate or inhibitor. pH variation has only a slight effect on fluorescence or anisotropy decay parameters, while dimethylsulfoxide appears to promote dissociation into monomers by weakening hydrophobic interaction between the subunits. The results are discussed in the light of newly developed insights into the functional role of rapid structural fluctuations in enzyme catalysis.     

Hydrophobic surfaces of tubulin probed by time-resolved and steady-state fluorescence of nile red

Binding of Nile Red to tubulin enhances and blue-shifts fluorescence emission to about 623 nm with a "shoulder" around 665 nm. Binding is reversible and saturable with an apparent Kd of approximately 0.6 microM. Nile Red does not alter tubulin polymerization, and polymerization in 2-(N-morpholino)ethanesulfonic acid (Mes) buffer does not alter the spectrum of the Nile Red-tubulin complex. In contrast, polymerization in glutamate buffer results in a red shift, reduction of intensity, and a decrease in lifetime, suggesting an increase in "polarity" of the binding environment. Lifetimes of 4.5 and 0.6 ns fluorescence in Mes buffer are associated with the 623-nm peak and the 665-nm shoulder, respectively. Indirect excitation spectra for these components are distinct and the 4.5-ns component exhibits tryptophan to Nile Red energy transfer. Acrylamide quenching yields linear Stern-Volmer plots with unchanged lifetimes, indicating static quenching. Apparent quenching constants are wavelength-dependent; global analysis reveals a quenchable component corresponding to the 4.5 ns component and an "unquenchable" component superposing the 0.6-ns spectrum. Analysis of anisotropy decay required an "associative" model which yielded rotational correlation times of greater than 50 ns for the 4.5-ns lifetime and 0.3 ns for the 0.6-ns lifetime. Dilution of tubulin in Mes results in an apparent red shift of emission without lifetime changes, due only to loss of the 623-nm component. These data are reconciled in terms of a model with two binding sites on the tubulin dimer. The more "nonpolar" site is located in a region of subunit-subunit contact which accounts for the fluorescence changes upon dilution; this permits estimation of a subunit dissociation constant of 1 microM.     

Thermal stability and ligand-binding properties of human plasma alpha 1-acid glycoprotein (orosomucoid) as determined with fluorescent probes

The fluorescence of 1,8-anilinonaphthalene sulfonate is enhanced and blue-shifted upon binding to alpha 1-acid glycoprotein, a human plasma protein of uncertain function. Fluorescence titrations of delipidated protein indicate at least two classes of binding sites having dissociation constants of 0.33 microM and 12 microM at 25 degrees C in 0.02 M potassium phosphate/0.15 M NaCl, pH 7.4. Exclusion chromatography measurements indicate only 1 binding site per mol protein, suggesting that the heterogeneity is due to differences between protein molecules, the origin of which remains unclear. The fluorescence of a mixture of dye and protein is progressively diminished upon addition of ethanol and other organic solvents whose presence could be detected at concentrations as low as 100 mM. Addition of the adrenergic drug propranolol to a mixture of alpha 1-acid glycoprotein (2.5 microM) and 1,8-anilinonaphthalene sulfonate (4 microM) caused a hyperbolic decrease in dye fluorescence to 30% of the initial value, with half-maximal response near 1 microM propranolol. When the protein-dye mixture was heated, the fluorescence of the dye exhibited a reversible downward transition with midpoint near 65 degrees C, compared to a midpoint of 58.5 degrees C obtained by intrinsic fluorescence in the absence of dye. This stabilization was confirmed with fluorescein-labeled protein, whose fluorescence polarization revealed a melting transition at 58.8 degrees C in the absence of ligands which increased by 5-6 Cdeg in the presence of 1,8-anilinonaphthalene sulfonate or propranolol. The sensitivity of 1,8-anilinonaphthalene sulfonate fluorescence to changes in the conformation and ligand environment of alpha 1-acid glycoprotein should facilitate efforts to understand the structure and function of this acute-phase reactant.     

Investigations of the effects of ethanol on warfarin binding to human serum albumin

Ethanol effects on warfarin binding to human serum albumin (HSA) have been studied by equilibrium dialysis and fluorescence methods at pH 7.4 in phosphate-buffered saline at 37 degrees C. In the presence of various amounts of ethanol fluorescence intensity of bound warfarin decreased significantly but this intensity reduction was not solely from displacement of bound warfarin from HSA. By comparing fluorescence and equilibrium dialysis data we concluded that fluorescence intensity reduction of warfarin was mainly the result of changes in the surrounding environment of the warfarin binding site by ethanol interaction with HSA and that displacement of bound warfarin was not significant compared to the fluorescence intensity changes. The dissociation constant of warfarin binding to HSA decreased with an increasing amount of ethanol. From the changes in fluorescence intensity upon warfarin binding to HSA with the presence of ethanol ranging from 0 to 5.0% the following dissociation constants (Kd) were determined: 0% ethanol 5.39 +/- 0.2 microM, 0.1% ethanol 5.86 +/- 0.1 microM, 0.3% ethanol 5.83 +/- 0.2 microM, 0.5% ethanol 6.76 +/- 0.1 microM, 1% ethanol 7.01 +/- 0.1 microM, 3% ethanol 9.9 +/- 0.7 microM, 5% ethanol 13.01 +/- 0.1 microM. From the equilibrium dialysis with the same ranges of ethanol presence the following Kd values were obtained: 0% ethanol 6. 62 +/- 1.6 microM, 0.1% ethanol 6.81 +/- 1.1 microM, 0.3% ethanol 8. 26 +/- 2.5 microM, 0.5% ethanol 8.86 +/- 1.9 microM, 1% ethanol 11. 01 +/- 4.2 microM, 3% ethanol 20.75 +/- 2.4 microM, 5% ethanol 21.67 +/- 2.2 microM. The results suggest that warfarin bound to HSA was displaced by ethanol. These data indicate that ethanol influence on warfarin binding to HSA may alter the pharmacokinetics of warfarin.     

The binding of 4',6-diamidino-2-phenylindole to bovine serum albumin.

The binding of 4',6-diamidino-2-phenylindole (DAPI) to bovine serum albumin (BSA) has been investigated between pH 6 and 8, in 0.05 M phosphate buffer at 20 degrees C, by fluorescence titrations and the results analyzed according to a procedure previously reported (R. Favilla and A. Mazzini, Biochim. Biophys. Acta 788 (1984) 48). The dye binds to the protein with a blue shift of about 4 nm in its fluorescence emission maximum, but with an enhancement factor of 10 of its fluorescence quantum yield. The dissociation constant decreases from 100 microM to 54 microM as the pH is increased from 6 to 8, with a constant number of nearly three equivalent binding sites. The complete displacement of DAPI bound to BSA by Ca2+ suggests a possible specificity of this substantially electrostatic interaction. The fluorescence decay of DAPI bound to the protein shows a double exponential kinetics, with a tau 1 = 0.97 ns and tau 2 = 2.78 ns. These results, compared with those obtained for DAPI alone, tau 1 = 0.16 ns and tau 2 = 2.8 ns, are rationalized in terms of two different rotamers of DAPI. Both rotamers are able to bind to the protein, but only one of them undergoes an intramolecular proton transfer, from the 6-amidinium group to the indole aromatic ring, in the excited singlet state of DAPI alone. When DAPI interacts with BSA this transfer does not occur and consequently a large increase of fluorescence is observed.(ABSTRACT TRUNCATED AT 250 WORDS)     

Mechanism of inhibition of Ca2+-transport activity of sarcoplasmic reticulum Ca2+-ATPase by anisodamine

The mechanism of inhibition of Ca2+-transport activity of rabbit sarcoplasmic reticulum Ca 2+-ATPase (SERCA) by anisodamine (a drug isolated from a medicinal herb Hyoscyamuns niger L) was investigated by using ANS (1-anilino-8-naphthalenesulfonate) fluorescence probe, intrinsic fluorescence quenching and Ca 2+-transport activity assays. The number of ANS binding sites for apo Ca2+-ATPase was determined as 8, using a multiple-identical binding site model. Both anisodamine and Ca2+ at millimolar level enhanced the ANS binding fluorescence intensities. Only anisodamine increased the number of ANS molecules bound by SERCA from 8 to 14. The dissociation constants of ANS to the enzyme without any ligand, with 30 mM anisodamine and with 15 mM Ca 2 were found to be 53.0 microM, 85.0 microM and 50.1 microM, respectively. Both anisodamine and Ca2+ enhanced the ANS binding fluorescenc with apparent dissociation constants of 7.6 mM and 2.3 mM, respectively, at a constant concentration of the enzyme. Binding of anisodamine significantly decreased the binding capacity of Ca2+ with the dissociation constant of 9.5 mM, but binding of Ca2+ had no obvious effect on binding of anisodamine. Intrinsic fluorescence quenching and Ca2+-transport activity assays gave the dissociation constants of anisodamine to SERCA as 9.7 and 5.4 mM, respectively, which were consistent with those obtained from ANS-binding fluorescence changes during titration of SERCA with anisodamine and anisodamine + 15 mM Ca2+, respectively. The results suggest that anisodamine regulates Ca2+-transport activity of the enzyme, by stabilizing the trans-membrane domain in an expanded, inactive conformation, at least at its annular ring region.     

Binding of nonsubstrate ligands to the glutathione S-transferases.

Fluorescence spectroscopy and inhibition kinetics were used to quantitate the affinity of nonsubstrate ligands for the rat liver glutathione S-transferases AA, A, B, and C in the presence of glutahione. The dissociation constants KD, for ligands such as bilirubin, indocyanine green, and hematin were determined by measuring the decrease in the intrinsic fluorescence of the proteins attendant on the addition of ligand. A second technique, used for compounds which absorb strongly at the excitation maxima of tryptophan, was to utilize 8-anilinonaphthalen sulfonate in the formation of protein complex fluorescing at a higher wavelength. The quenching of this complex allowed the determination of the dissociation constants for ligands such as 3,6-dibromosulfophthalein and cephalothin. These data indicate that all four proteins bind these ligands but do so with different affinities. The bilirubin-induced decrease in fluorescence was used to estimate the stoichiometry of binding as 1.2 mol of bilirubin bound/mol of transferase B and 0.7 mol/mol of transferase C. All of the ligands examine are inhibitors of catalytic activity, as tested in a standard assay with GSH and 1-chloro-2,4-dinitrobenzene as substrates. From these studies we conclude that these proteins have a broad specificity not only for their substrates, but for the binding of nonsubstrate ligands as well.     

Recognition and Binding of a Helix-Loop-Helix Peptide to Carbonic Anhydrase Occurs via Partly Folded Intermediate Structures

We have studied the association of a helix-loop-helix peptide scaffold carrying a benzenesulfonamide ligand to carbonic anhydrase using steady-state and time-resolved fluorescence spectroscopy. The helix-loop-helix peptide, developed for biosensing applications, is labeled with the fluorescent probe dansyl, which serves as a polarity-sensitive reporter of the binding event. Using maximum entropy analysis of the fluorescence lifetime of dansyl at 1:1 stoichiometry reveals three characteristic fluorescence lifetime groups, interpreted as differently interacting peptide/protein structures. We characterize these peptide/protein complexes as mostly bound but unfolded, bound and partly folded, and strongly bound and folded. Furthermore, analysis of the fluorescence anisotropy decay resulted in three different dansyl rotational correlation times, namely 0.18, 1.2, and 23 ns. Using the amplitudes of these times, we can correlate the lifetime groups with the corresponding fluorescence anisotropy component. The 23-ns rotational correlation time, which appears with the same amplitude as a 17-ns fluorescence lifetime, shows that the dansyl fluorophore follows the rotational diffusion of carbonic anhydrase when it is a part of the folded peptide/protein complex. A partly folded and partly hydrated interfacial structure is manifested in an 8-ns dansyl fluorescence lifetime and a 1.2-ns rotational correlation time. This structure, we believe, is similar to a molten-globule-like interfacial structure, which allows segmental movement and has a higher degree of solvent exposure of dansyl. Indirect excitation of dansyl on the helix-loop-helix peptide through Förster energy transfer from one or several tryptophans in the carbonic anhydrase shows that the helix-loop-helix scaffold binds to a tryptophan-rich domain of the carbonic anhydrase. We conclude that binding of the peptide to carbonic anhydrase involves a transition from a disordered to an ordered structure of the helix-loop-helix scaffold.     

Time-resolved fluorescence spectroscopy of lumazine protein from Photobacterium phosphoreum using synchrotron radiation

Time-resolved fluorescence on lumazine protein from Photobacterium phosphoreum was performed with synchrotron radiation as a source of continuously tunable excitation. The experiments yielded structural and dynamic details from which two aspects became apparent. From fluorescence anisotropy decay monitoring of lumazine fluorescence with different excitation wavelengths, the average correlation times were shown to change, which must indicate the presence of anisotropic motion of the protein. A similar study with 7-oxolumazine as the fluorescent ligand led to comparable results. The other remarkable observation dealt with the buildup of acceptor fluorescence, also observed with 7-oxolumazine although much less pronounced, which is caused by the finite energy transfer process between the single donor tryptophan and the energy accepting lumazine derivatives. Global analytical approaches in data analysis were used to yield realistic correlation times and reciprocal transfer rate constants. It was found that the tryptophan residue has a large motional freedom as also reported previously for this protein and for the related protein from P. leiognathi (Lee et al. 1985; Kulinski et al. 1987). The average distance between the tryptophan residue and the ligand donor-acceptor couple has been determined to be 2.7 nm for the same donor and two different acceptors.     

New insight on beta-lactoglobulin binding sites by 1-anilinonaphthalene-8-sulfonate fluorescence decay

The fluorescence time decay parameters of the beta-lactoglobulin-1-anilinonaphthalene-8-sulfonate complex have been investigated under physical and chemical perturbations (2 < pH < 8 and added electrolyte 0 < NaCl < 0.5 M) to obtain new insight on the nature of the protein binding interactions. A double exponential decay of the bound probe lifetime has been confirmed by the presence of a longer component, 11 to 14.5 ns, and a shorter component, 2.5 to 3.5 ns. The two lifetimes are ascribed to different binding modes associated also with different exposure to the solvent; in particular, the longer component is attributed to binding inside the hydrophobic beta barrel, while a "surface" site is suggested for the shorter component. A detailed analysis of the lifetime fractional intensities correlates the binding constants with ionic strength and supports the presence of electrostatic effects at both sites. A Debye-Hückel approach, applied to extrapolate the electrostatic free energy contribution vs. pH at vanishing ionic strength, gives interesting clues on the effective charge felt by the ANS ligands in the proximity of each site. In particular, binding is found to parallel the aspartate and glutamate titrations between pH 3 and pH 4.5; the "surface" site mainly responds to the presence of these local titrating charges while the "internal" site more closely follows the overall protein net charge.     

An oxygenation-sensitive dye binding to Carcinus maenas hemocyanin

The interaction of 4',6-diamidino-2-phenylindole (DAPI) with Carcinus maenas hemocyanin has been investigated by steady state fluorescence, dynamic fluorescence and circular dichroism measurements. The dye binds to apohemocyanin (without copper) as well as to oxygenated hemocyanin and to deoxygenated hemocyanin with very similar affinities (kd approximately equal to 1 microM ) and number of binding sites (one per subunit). In contrast, the fluorescence quantum yield enhancement of DAPI bound to oxygenated hemocyanin is nearly 60% lower than that observed for deoxygenated and apo forms. The decrease of fluorescence of the dye bound to deoxygenated hemocyanin is a sigmoidal function of the oxygen partial pressure, specular to that observed by following the absorbance of the copper-oxygen charge transfer band at 340 nm. This result provides preliminary evidence that DAPI may be used as a functional probe to monitor the cooperative binding of oxygen to the protein. The higher fluorescence quantum yield of DAPI bound to either apohemocyanin or deoxygenated protein is characterized by a single fluorescence decay with lifetime of about 3 ns, while with the oxygenated protein two components of about 1 ns and 3.0 ns are observed. This result is interpreted assuming the existence of two rotamers of DAPI in solution (Szabo et al. Photochem. Photobiol. 44 (1986) 143-150) both able to interact with oxygenated hemocyanin but only one to deoxygenated and apo forms. We conclude that the different fluorescence behaviour of the dye induced by the presence of oxygen bound to the protein is probably due to a structural change of hemocyanin in cooperative interaction with oxygen. Furthermore, the interaction is confirmed by the induced negative ellipticity of DAPI bound to apohemocyanin and deoxy-hemocyanin and by the increase of fluorescence anisotropy of DAPI bound to all forms of protein investigated.