Rotational freedom of tryptophan residues in proteins and peptides

We studied the rotational motions of tryptophan residues in proteins and peptides by measurement of steady-state fluorescence anisotropies under conditions of oxygen quenching. By fluorescence quenching we can shorten the fluorescence lifetime and thereby decrease the average time for rotational diffusion prior to fluorescence emission. This method allowed measurement of rotational correlation times ranging from 0.03 to 50 ns, when the unquenched fuorescence lifetimes are near 4 ns. A wide range of proteins and peptides were investigated with molecular weights ranging from 200 to 80 000. Many of the chosen substances possessed a single tryptophan residue to minimize the uncertainties arising from a heterogeneous population of fluorophores. In addition, we also studied a number of multi-tryptophan proteins. Proteins were studied at various temperatures, under conditions of self-association, and in the presence of denaturants. A wide variety of rotational correlation times were found. As examples we note that the single tryptophan residue of myelin basic protein was highly mobile relative to overall protein rotation whereas tryptophan residues in human serum albumin, RNase T1, aldolase, and horse liver alcohol dehydrogenase were found to be immobile relative to the protein matrix. These results indicate that one cannot generalize about the extent of segmental mobility of the tryptophan residues in proteins. This physical property of proteins is highly variable between proteins and probably between different regions of the same protein.     

Application of a reference convolution method to tryptophan fluorescence in proteins. A refined description of rotational dynamics

A reference method for the deconvolution of polarized fluorescence decay data is described. Fluorescence lifetime determinations for p-terphenyl, p-bis[2-(5-phenyloxazolyl)]benzene and N-acetyltryptophanamide (AcTrpNH2) show that with this method more reliable fits of the decays can be made than with the scatterer method, which is most frequently used. Analysis of the AcTrpNH2 decay with p-terphenyl as the reference compound yields an excellent fit with lifetimes of 2.985 ns for AcTrpNH2 and 1.099 ns for p-terphenyl (20 degrees C), whereas the AcTrpNH2 decay cannot be satisfactorily fitted when the scatterer method is used. The frequency of the detected photons is varied to determine the conditions where pulse pile-up starts to affect the measured decays. At detection frequencies of 5 kHz and 15 kHz, which corresponds to 1.7% and 5% respectively of the rate of the excitation photons no effects are found. Decays measured at 30 kHz (10%) are distorted, indicating that pile-up effects play a role at this frequency. The fluorescence and fluorescence anisotropy decays of the tryptophan residues in the proteins human serum albumin, horse liver alcohol dehydrogenase and lysozyme have been reanalysed with the reference method. The single tryptophan residue of the albumin is shown to be characterized by a triple-exponential fluorescence decay. The anisotropy decay of albumin was found to be mono-exponential with a rotational correlation time of 26 ns (20 degrees C). The alcohol dehydrogenase has two different tryptophan residues to which single lifetimes are assigned. It is found that the rotational correlation time for the dehydrogenase changes with excitation wavelength (33 ns for lambda ex = 295 nm and 36 ns for lambda ex = 300 nm at 20 degrees C), indicating a nonspherical protein molecule. Lysozyme has six tryptophan residues, which give rise to a triple-exponential fluorescence decay. A single-exponential decay with a rotational correlation time of 3.8 ns is found for the anisotropy. This correlation time is significantly shorter than that arising from the overall rotation and probably originates from intramolecular, segmental motion.     

Correlation between internal motion and emission kinetics of tryptophan residues in proteins

Time-resolved fluorescence anisotropy measurements of tryptophan residues were carried out for 44 proteins. Internal rotational motion with a sub-nanosecond correlation time (0.9 +/- 0.6 ns at 10 degrees C) was seen in a large number of proteins, though its amplitude varied from protein to protein. It was found that tryptophan residues which were almost fixed within a protein had either a long (greater than 4 ns) or short (less than 2 ns) fluorescence lifetime, whereas a residue undergoing a large internal motion had an intermediate lifetime (1.5-3 ns). It is suggested that the emission kinetics of a tryptophan residue is coupled with its internal motion. In particular, an immobile tryptophan residue emitting at long wavelength was characterized by a long lifetime (greater than 4 ns). It appears that a tryptophan residue fixed in a polar region has little chance of being quenched by neighboring groups.     

Quenching-resolved emission anisotropy studies with single and multitryptophan-containing proteins

Measurements of the anisotropy of protein fluorescence as a function of an added collisional quencher, such as acrylamide, are used to construct Perrin plots. For single tryptophan containing proteins, such plots yield an apparent rotational correlation time for the depolarization process, which, in most cases, is approximately the value expected for Brownian rotation of the entire protein. Apparent limiting fluorescence anisotropy values, which range from 0.20 to 0.32 for the proteins studied, are also obtained from the Perrin plots. The lower values for the limiting anisotropy found for some proteins are interpreted as indicating the existence of relatively rapid, limited (within a cone of angle 0 degrees--30 degrees) motion of the tryptophan side chains that is independent of the overall rotation of the protein. Examples of the use of this fluorescence technique to study protein conformational changes are presented, including the monomer in equilibrium dimer equilibrium of beta-lactoglobulin, the monomer in equilibrium tetramer equilibrium of melittin, the N in equilibrium F transition of human serum albumin, and the induced change in the conformation of cod parvalbumin caused by the removal of Ca+2. Because multitryptophan-containing proteins have certain tryptophans that are accessible to solute quencher and others that are inaccessible, this method can be used to determine the steady state anisotropy of each class of tryptophan residues.     

Nanosecond motions of the single tryptophan residues in apolipoproteins C-I and C-II: a study by oxygen quenching and fluorescence depolarization

Rotational freedom of the single tryptophan residue in human plasma apolipoproteins C-I (apo C-I) and C-II (apo C-II) was investigated by oxygen quenching and lifetime-resolved anisotropies. The tryptophan in both apo C-I and C-II was highly accessible to oxygen quenching. The tryptophan residue in both apo C-I and C-II and their sodium dodecyl sulfate (SDS) or dimyristoylphosphatidylcholine (DMPC) complexes displayed significant motional freedom on the nanosecond time scale. Lifetime-resolved anisotropies of tryptophan residues under conditions of oxygen quenching revealed an increase in the amplitude of the segmental motions at 40 degrees C as compared to that at 5 degrees C. It was concluded from these studies that both the apoprotein C-I and C-II are highly flexible molecules, and that the nanosecond motions of the tryptophan residue are sensitive to the fluidity of its environment in both SDS and DMPC complexes.     

Effect of ligand binding and conformational changes in proteins on oxygen quenching and fluorescence depolarization of tryptophan residues

The rotational freedom of tryptophan residues in protein-ligand complexes was studied by measuring steady-state fluorescence anisotropies under conditions of oxygen quenching. There was a decrease in the oxygen bimolecular quenching constant upon complexation of trypsin and alpha-chymotrypsin with proteinaceous trypsin inhibitors, of lysozyme with N-acetylglucosamine (NAG) and di(N-acetyl-D-glucosamine) ((NAG)2) and of hexokinase with glucose. Binding of the bisubstrate analogue N-phosphonacetyl-L-aspartate (PALA) to aspartate transcarbamylase (ATCase) and binding of biotin to avidin resulted in increased oxygen quenching constants. The tryptophan of human serum albumin (HSA) in the F state was more accessible to oxygen quenching than that in the N state. With the exception of ATCase, the presence of subnanosecond motions of the tryptophan residues in all the proteins is suggested by the short apparent correlation times for fluorescence depolarization and by the low apparent anisotropies obtained by extrapolation to a lifetime of zero. Complex formation evidently resulted in more rigid structures in the case of trypsin, alpha-chymotrypsin and lysozyme. The effects of glucose binding on hexokinase were not significant. Binding of biotin to avidin resulted in a shorter correlation time for the tryptophan residues. The N --> F transition in HSA resulted in a more rigid environment for the tryptophan residue. Overall, these changes in the dynamics of the protein matrix and motional freedom of tryptophan residues due to complex formation and subsequent conformational changes are in the same direction as those observed by other techniques, especially hydrogen exchange. Significantly, the effects of complex formation on protein dynamics are variable. Among the limited number of cases we examined, the effects of complex formation were to increase, decrease or leave unchanged the apparent dynamics of the protein matrix.     

Enhanced resolution of fluorescence anisotropy decays by simultaneous analysis of progressively quenched samples. Applications to anisotropic rotations and to protein dynamics.

Enhanced resolution of rapid and complex anisotropy decays was obtained by measurement and analysis of data from progressively quenched samples. Collisional quenching by acrylamide was used to vary the mean decay time of indole or of the tryptophan fluorescence from melittin. Anisotropy decays were obtained from the frequency-response of the polarized emission at frequencies from 4 to 2,000 MHz. Quenching increases the fraction of the total emission, which occurs on the subnanosecond timescale, and thereby provides increased information on picosecond rotational motions or local motions in proteins. For monoexponential subnanosecond anisotropy decays, enhanced resolution is obtained by measurement of the most highly quenched samples. For complex anisotropy decays, such as those due to both local motions and overall protein rotational diffusion, superior resolution is obtained by simultaneous analysis of data from quenched and unquenched samples. We demonstrate that measurement of quenched samples greatly reduces the uncertainty of the 50-ps correlation time of indole in water at 20 degrees C, and allows resolution of the anisotropic rotation of indole with correlation times of 140 and 720 ps. The method was applied to melittin in the monomeric and tetrameric forms. With increased quenching, the anisotropy data showed decreasing contributions from overall protein rotation and increased contribution from picosecond tryptophan motions. The tryptophan residues in both the monomeric and the tetrameric forms of melittin displayed substantial local motions with correlation times near 0.16 and 0.06 ns, respectively. The amplitude of the local motion is twofold less in the tetramer. These highly resolved anisotropy decays should be valuable for comparison with molecular dynamics simulations of melittin.     

Time-resolved fluorescence of the single tryptophan residue in rat alpha-fetoprotein and rat serum albumin: analysis by the maximum-entropy method.

The time-resolved fluorescence emissions of the lone tryptophan residues in rat alpha-fetoprotein (RFP) and rat serum albumin (RSA) were studied. The total fluorescence intensity decays in both proteins were multiexponential. Analysis of the data by nonlinear least squares as a sum of discrete exponentials showed that four exponentials were needed for a satisfactory fit for both proteins. Analysis by the maximum entropy method using 150 logarithmically equally spaced exponentials yielded four well-resolved excited-state lifetime classes with barycenters and relative amplitudes values (ci) that corresponded to those obtained from the nonlinear least-squares method. Changing the temperature affected the relative amplitudes of the lifetime classes but had little effect on the lifetime values themselves. This suggests that the four classes reflect local conformational substates that exchange slowly with respect to the time window of observation defined by the longest lifetime. The internal rotational dynamics of the tryptophan in each protein was monitored by fluorescence anisotropy decay measurements. The mobility of the tryptophan appeared to be larger and faster in RFP than in RSA. The nonlinear least-squares analysis suggests the existence of three rotational correlation times of 0.1, 3, and 55 ns for this protein. As a function of temperature, the long correlation time did not follow the Perrin's law expected for a rigid rotating body. This suggests that this correlation time may reflect not only the Brownian rotation of the whole protein but also the flexibilities of domains in the protein. For RSA a two-component model with correlation times of 0.4 and 31 ns was sufficient to describe the data.(ABSTRACT TRUNCATED AT 250 WORDS)     

The fluorescence decay of tryptophan residues in native and denatured proteins.

The fluorescence decay kinetics at different ranges of the emission spectrum is reported for 17 proteins. Out of eight proteins containing a single tryptophan residue per molecule, seven proteins display multiexponential decay kinetics, suggesting that variability in protein structure may exist for most proteins. Tryptophan residues whose fluorescence spectrum is red shifted may have lifetimes longer than 7 ns. Such long lifetimes have not been detected in any of the denatured proteins studied, indicating that in native proteins the tryptophans having a red-shifted spectrum are affected by the tertiary structure of the protein. The fluorescence decay kinetics of ten denatured proteins studied obey multiexponential decay functions. It is therefore concluded that the tryptophan residues in denatured proteins can be grouped in two classes. The first characterized by a relatively long lifetime of about 4 ns and the second has a short lifetime of about 1.5 ns. The emission spectrum of the group which is characterized by the longer lifetime is red shifted relative to the emission spectrum of the group characterized by the shorter lifetime. A comparison of the decay data with the quantum yield of the proteins raises the possibility that a subgroup of the tryptophan residues is fully quenched. It is noteworthy that despite this heterogeneity in the environment of tryptophan residues in each denatured protein, almost the same decay kinetics has been obtained for all the denatured proteins studied in spite of the vastly different primary structures. It is therefore concluded that each tryptophan residue interacts in a more-or-less random manner with other groups on the polypeptide chain, and that on the average the different tryptophan residues in denatured proteins have a similar type of environment.     

Nanosecond dynamics of tryptophans in different conformational states of apomyoglobin proteins

Fluorescence anisotropy kinetics were employed to quantify the nanosecond mobility of tryptophan residues in different conformational states (native, molten globule, unfolded) of apomyoglobins. Of particular interest is the similarity between the fluorescence anisotropy decays of tryptophans in the native and molten globule states. We find that, in these compact states, tryptophan residues rotate rapidly within a cone of semiangle 22-25 degrees and a correlation time of 0.5 ns, in addition to rotating together with the whole protein with a correlation time of 7-11 ns. The similar nanosecond dynamics of tryptophan residues in both states suggests that the conformation changes that distinguish the molten globule and native states of apomyoglobins originate from either subtle, slow rearrangements or fast changes distant from these tryptophans.     

Ligand binding and protein dynamics: a fluorescence depolarization study of aspartate transcarbamylase from Escherichia coli

The polarization of the fluorescence and the real-time fluorescence intensity decay of the two tryptophan residues of aspartate transcarbamylase from Escherichia coli were studied as a function of temperature. The protein was dissolved in an 80% glycerol/buffer mixture, and temperatures were varied between -40 and 20 degrees C in order to limit the depolarization to local rotations of the tryptophans. Two fluorescent species contribute to over 95% of the emission. They differ in their fluorescence lifetimes by approximately 4 ns depending upon the temperature observed and their fractional contributions to the total intensity. The Y-plot analysis of the polarization and lifetime data allows for the distinction of two rotational species by their critical amplitude of rotation, the first being component 1 and the second being component 2. We suggest that these two species correspond to the two tryptophan residues of the protein. The polarization and lifetime experiments were carried out for ATCase in presence of the bisubstrate analogue N-(phosphonoacetyl)-L-aspartate (PALA) and in presence of the nucleotide effector molecules ATP and CTP. The binding of PALA results in an increase in the thermal coefficient of frictional resistance to rotation of tryptophan 1 and a decrease in that of tryptophan 2. ATP binding does not affect the degree to which the protein hinders tryptophan rotation but does result in a change in the critical amplitude of rotation of tryptophan 2. The results obtained in the presence of CTP are similar to those obtained with PALA.     

Fluorescence lifetime and spectral study of the acid expansion of bovine serum albumin

The fluorescence lifetimes of the tryptophan residues of bovine serum albumin were measured in the native and acid-expanded conformation. A three-exponential process is required to fit the fluorescence decay data. The results are interpreted empirically in terms of two emitting species. The emission at longer wavelength (360 nm) has slower rates of decay than that at shorter wavelength (325 nm). For both emitting species the average lifetime decreases when the N-F transition occurs and shortens further when the protein expands. Rotational correlation times, derived from the decay of the fluorescence anisotropy of the tryptophan residues, suggest that longer emission wavelengths are associated with somewhat shorter correlation times. There is no certain indication of any independent motion of the tryptophans in any conformation, although some very fast process, perhaps Raman scattering, appears to occur. On acid expansion the long correlation times decrease to around 10 ns in the fully expanded form. Static quenching experiments using I- or acrylamide suggest a greater average exposure of the tryptophans when the protein is most greatly expanded. This is despite the fact that the fluorescence emission maximum shifts to shorter wavelength under these conditions. Also, there is no difference in accessibility to quenching between the longer and shorter wavelength emissions.     

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)     

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.     

Time-resolved fluorescence study of human recombinant interferon alpha 2. Association state of the protein, spatial proximity of the two tryptophan residues.

Human recombinant interferon alpha 2 belongs a to family of proteins active against a wide range of viruses. It contains two tryptophan residues located at positions 77 and 141 in the peptide sequence. The fluorescence emission spectrum of these tryptophan residues displays a maximum at 335 nm. The fluorescence intensity decay is described by one broad excited-state-lifetime population centered around a value of 1.7 ns (full width at half maximum, 1.5 ns). These observations suggest that in the native protein, both tryptophan residues emit from similar environments, not directly exposed to the surrounding solvent. The anisotropy decay is essentially biexponential. The correlation-time value characterizing the Brownian rotation of the protein varies linearly with the viscosity/temperature ratio. The calculated hydrodynamic volumes are compatible with the existence of a dimer and a tetramer, at pH 5.5 and 9.4, respectively. Addition of urea at pH 5.5 disrupts the dimer and modifies to some extent the excited-state-lifetime distribution which becomes more heterogeneous. Disulfide-bond reduction also dissociates the dimer and leads to a highly heterogeneous fluorescence-intensity decay with four excited-state-lifetime populations. An opening of the local structure in the Trp region of the protein is likely to occur in these conditions. The fast-anisotropy-decay components can be due to either fast rotation or energy transfer between the indoles. Close proximity of the two Trp residues (less than 1 nm) is suggested from steady-state and time-resolved fluorescence-anisotropy measurements in vitrified medium [95% (by mass) glycerol at -38 degrees C]. This suggestion is in agreement with the recently published three-dimensional structure of the homologous protein murine interferon beta [Senda, T., Shimazu, T., Matsuda, S. Kawano, G., Shimizu, H., Nakamura, K. T. & Mitsui, Y. (1992) EMBO J. 11, 3193-3201].     

The effects of ligands on the conformation of phosphoglycerate kinase: fluorescence anisotropy decay and theoretical interpretation

Horse muscle phosphoglycerate kinase (PGK) is a monomer folded into two widely distant domains. In the glycolytic pathway, this enzyme catalyzes the first reaction that produces ATP. It was suggested, by analogy with yeast hexokinase, that a hinge-bending motion may be induced by the binding of specific substrates to the protein. To analyze such a motion, or any structural changes induced by ligand binding, fluorescence anisotropy decay of tryptophan residues in free and liganded PGK was studied. At 293 K, for the free protein and the binary complex with 3-phosphoglycerate, a single correlation time of 26 ns was observed, corresponding to the rotation of the overall protein, whereas upon addition of MgADP, this correlation time decreased to 10 ns. Such a decrease cannot be merely due to a change of the protein's shape and volume. To explain this, it was suggested that the fluorescence anisotropy decay of the PGK-MgADP complex corresponded to the rotation of the only buried tryptophan (Trp 335). The rotational paths of this tryptophan, in the presence and absence of the nucleotide, were established by potential energy minimization calculations. The results indicated that MgADP induces a displacement of helix alpha-13 that decreases the rotational energy barrier of Trp 335 from 16 kcal/mol in the free protein to 8 kcal/mol in the complex.     

Structure and dynamics of the alpha-lactalbumin molten globule: fluorescence studies using proteins containing a single tryptophan residue

The fluorescence properties of three variants of alpha-lactalbumin (alpha-LA) containing a single tryptophan residue were investigated under native, molten globule, and unfolded conditions. These proteins have levels of secondary structure and stability similar to those of the wild type. The fluorescence signal in the native state is dominated by that of W104, with the signal of W60 and W118 significantly quenched by the disulfide bonds in their vicinity. In the molten globule state, the magnitude of the fluorescence signal of W60 and W118 increases, due to the loss of rigid, specific side chain packing. In contrast, the magnitude of the signal of W104 decreases in the molten globule state, perhaps due to the protonation of H107 or quenching by D102 or K108. The solvent accessibilities of individual tryptophan residues were investigated by their fluorescence emission maximum and by acrylamide quenching studies. In the native state, the order of solvent accessibility is as follows: W118 > W60 > W104. This order changes to W60 > W104 > W118 in the molten globule state. Remarkably, the solvent accessibility of W118 in the alpha-LA molten globule is lower than that in the native state. The dynamic properties of the three tryptophan residues were examined by time-resolved fluorescence anisotropy decay studies. The overall rotation of the molecule can be observed in both the native and molten globule states. In the molten globule state, there is an increase in the extent of local backbone fluctuations with respect to the native state. However, the fluctuation is not sufficient to result in complete motional averaging. The three tryptophan residues in the native and molten globule states have different degrees of motional freedom, reflecting the folding pattern and dynamic heterogeneity of these states. Taken together, these studies provide new insight into the structure and dynamics of the alpha-LA molten globule, which serves as a prototype for partially folded proteins.     

Time-resolved tryptophan fluorescence anisotropy investigation of bacteriophage M13 coat protein in micelles and mixed bilayers

Coat protein of bacteriophage M13 is examined in micelles and vesicles by time-resolved tryptophan fluorescence and anisotropy decay measurements and circular dichroism experiments. Circular dichroism indicates that the coat protein has alpha-helix (60%) and beta-structure (28%) in 700 mM sodium dodecyl sulfate micelles and predominantly beta-structure (94%) in mixed dimyristoylphosphatidylcholine/dimyristoylphosphatidic acid (80/20 w/w) small unilamellar vesicles. The fluorescence decay at 344 nm of the single tryptophan in the coat protein after excitation at 295 or 300 nm is a triple exponential. In the micelles the anisotropy decay is a double exponential. A short, temperature-independent correlation time of 0.5 +/- 0.2 ns reflects a rapid depolarization process within the coat protein. The overall rotation of the coat protein-detergent complex is observed in the decay as a longer correlation time of 9.8 +/- 0.5 ns (at 20 degrees C) and has a temperature dependence that satisfies the Stokes-Einstein relation. In vesicles at all lipid to protein molar ratios in the range from 20 to 410, the calculated order parameter is constant with a value of 0.7 +/- 0.1 from 10 to 40 degrees C, although the lipids undergo the gel to liquid-crystalline phase transition. The longer correlation time decreases gradually on increasing temperature. This effect probably arises from an increasing segmental mobility within the coat protein. The results are consistent with a model in which the coat protein has a beta-structure and the tryptophan indole rings do not experience the motion of the lipids in the bilayer because of protein-protein aggregation.     

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).     

Effects of temperature on the fluorescence intensity and anisotropy decays of staphylococcal nuclease and the less stable nuclease-conA-SG28 mutant

Frequency-domain fluorescence spectroscopy was used to investigate the effects of temperature on the intensity and anisotropy decays of the single tryptophan residues of Staphylococcal nuclease A and its nuclease-conA-SG28 mutant. This mutant has the beta-turn forming hexapeptide, Ser-Gly-Asn-Gly-Ser-Pro, substituted for the pentapeptide Tyr-Lys-Gly-Gln-Pro at positions 27-31. The intensity decays were analyzed in terms of a sum of exponentials and with Lorentzian distributions of decay times. The anisotropy decays were analyzed in terms of a sum of exponentials. Both the intensity and anisotropy decay parameters strongly depend on temperature near the thermal transitions of the proteins. Significant differences in the temperature stability of Staphylococcal nuclease and the mutant exist; these proteins show characteristic thermal transition temperatures (Tm) of 51 and 30 degrees C, respectively, at pH 7. The temperature dependence of the intensity decay data are shown to be consistent with a two-state unfolding model. For both proteins, the longer rotational correlation time, due to overall rotational diffusion, decreases dramatically at the transition temperature, and the amplitude of the shorter correlation time increases, indicating increased segmental motions of the single tryptophan residue. The mutant protein appears to have a slightly larger overall rotational correlation time and to show slightly more segmental motion of its Trp than is the case for the wild-type protein.