Frequency-domain fluorescence studies of an extracellular metalloproteinase of Staphylococcus aureus

A frequency-domain fluorescence study of calcium-binding metalloproteinase from Staphylococcus aureus has shown that this two-tryptophan-containing protein exhibits a double-exponential fluorescence decay. At 10 degrees C in 0.05 M Tris-HCl buffer (pH 9.0) containing 10 mM CaCl2, fluorescence lifetimes of 1.2 and 5.1 ns are observed. Steady-state and frequency-domain solute-quenching studies are consistent with the assignment of the two lifetimes to the two tryptophan residues. The tryptophan residue characterized by a shorter lifetime has a maximum of fluorescence emission at about 317 nm and the second one exhibits a maximum of its emission at 350 nm. These two residues contribute almost equally to the protein's fluorescence. These results, as well as fluorescence-quenching studies using KI and acrylamide as a quencher, indicate that in calcium-loaded metalloproteinase, the tryptophan residue characterized by the shorter lifetime is extensively buried within the protein. The second residue is exposed on the surface of the protein. The tryptophan residues of metalloproteinase have acrylamide dynamic-quenching rate constants, kq values, of 2.3 and 0.26 X 10(9) M-1 X s-1 for the exposed and buried residue, respectively. A study of the temperature dependence of the fluorescence lifetime for the two tryptophan components gives activation energies, Ea values, for thermal quenching of 1.8 and 2.2 kcal/mol for the buried and the exposed residue, respectively. Dissociation of Ca2+ from the protein causes a change in the protein's structure, as can be judged from dramatic changes which occur in the fluorescence properties of the buried tryptophan residue. These changes include an approx. 13 nm red-shift in the maximum of the fluorescence emission and an increase in the acrylamide-quenching rate constant, and they indicate that the removal of Ca2+ results in an increase in the exposure and the polarity of the microenvironment of this 'blue' residue.     

Internal motion and electron transfer in proteins: a picosecond fluorescence study of three homologous azurins

We have carried out a picosecond fluorescence study of holo- and apoazurins of Pseudomonas aeruginosa (azurin Pae), Alcaligenes faecilis (azurin Afe), and Alcaligenes denitrificans (azurin Ade). Azurin Pae contains a single, buried tryptophyl residue; azurin Afe, a single surface tryptophyl residue; and azurin Ade, tryptophyl residues in both environments. From anisotropy measurements we conclude that the interiors of azurins Pae and Ade are not mobile enough to enable motion of the indole ring on a nanosecond time scale. The exposed tryptophans in azurins Afe and Ade show considerable mobility on a few hundred picosecond time scale. The quenching of tryptophan fluorescence observed in the holoproteins is interpreted in terms of electron transfer from excited-state tryptophan to Cu(II). The observed rates are near the maximum predicted by Marcus theory for the separation of donor and acceptor. The involvement of protein matrix and donor mobility for electron transfer is discussed. The two single-tryptophan-containing proteins enable the more complex fluorescence behavior of the two tryptophans of azurin Ade to be understood. The single-exponential fluorescence decay observed for azurin Pae and the nonexponential fluorescence decay observed for azurin Afe are discussed in terms of current models for tryptophan photophysics.     

A spectrofluorometric study of the environment of tryptophans in bacteriorhodopsin

The emission spectrum of intact purple membranes of Halobacterium halobium has a very short wavelength position (the main maximum at 314 nm) and can be fitted by two spectral components, one of which (component A) corresponds to the fluorescence of buried tryptophan residues located in a highly hydrophobic rigid environment (like the single tryptophan residue in azurin), the other (component I) being due to the emission of buried tryptophan residues located in a rather polar environment. Treatment of bacteriorhodopsin by NaBH4, fragmentation of the membranes and thermal formation of vesicles result in a decrease in the contribution of component A, an increase in that of component I and the appearance of spectral components corresponding to the emission of surface tryptophan residues. Temperature induces at least two distinct changes of the fluorescence parameters of the protein: one change occurs from 45 to 65 degrees C. the other from 65 to 90 degrees C. The spectral changes correlate with the peaks of heat sorption caused by thermal transitions in the purple membrane structure and conformational changes in the protein structure. Alkaline denaturation of bacteriorhodopsin registered by tryptophan fluorescence begins at pH > 11.0.     

Homogeneity and variability in the structure of azurin molecules studied by fluorescence decay and circular polarization.

The fluorescence decay of apoazurin derived from Pseudomonas aeruginosa is monoexponential. By this criterion the population of molecules of apoazurin is homogeneous. The emission anisotropy factor and the absorption anisotropy factor at the red edge of the absorption band assume similar values, showing that the tryptophan residue in apoazurin has the same asymmetric environment both in the ground and excited states. This finding suggests tight packing of the protein at the tryptophan environment. Native azurin does not decay monoexponentially. Moreover, comparison between the quantum yield calculated from the decay kinetics and the one measured directly shows that the majority of the azurin molecules are not fluorescent. There is thus variability in the structure of azurin molecules with an equilibration time that is longer than the fluorescence lifetime. Different asymmetric environment was found for the tryptophan residue in oxidized and reduced holoprotein and in apoazurin, as studied by the circular polarization of the fluorescence. D(2)O increases the fluorescence lifetime of apoazurin by 6 percent, compared to the lifetime in H(2)O solution; therefore water molecules may have access to the tryptophan residue, though the latter is situated in a hydrophobic environment.     

Conformational heterogeneity of the copper binding site in azurin. A time-resolved fluorescence study.

Comparison of the fluorescence spectra and the effect of temperature on the quantum yields of fluorescence of Azurin (from Pseudomonas fluorescens ATCC-13525-2) and 3-methylindole (in methylcyclohexane solution) provides substantive evidence that the tryptophan residue in azurin is completely inaccessible to solvent molecules. The quantum yields of azurin (CuII), azurin (CuI), and apoazurin (lambda ex = 291 nm) were 0.052, 0.054, and 0.31, respectively. Other evidence indicates that there is no energy transfer from tyrosine to tryptophan in any of these proteins. The fluorescence decay behavior of each of the azurin samples was found to be invariant with emission wavelength. The fluorescences of azurin (CuII) and azurin (CuI) decay with dual exponential kinetics (tau 1 = 4.80 ns, tau 2 = 0.18 ns) while that of apoazurin obeys single exponential decay kinetics (tau = 4.90). The ratio of pre-exponentials of azurin (CuII), alpha 1/alpha 2, is found to be 0.25, and this ratio increases to 0.36 on reduction to azurin (CuI). The results are interpreted as originating from different interactions of the tryptophan with two conformers of the copper-ligand complex in azurin.     

Time-resolved fluorescence study of azurin variants: conformational heterogeneity and tryptophan mobility.

Time-resolved fluorescence and time resolved fluorescence anisotropy studies have been performed on wild-type azurin from Pseudomonas aeruginosa and two variants to study the mobility of Trp48. The two azurin variants in which the microenvironment of Trp48 was changed comprised the single mutations Ile7Ser and Phe110Ser. The experiments were performed on the holo-Cu(I), holo-Cu(II), and apo- forms at various pH values, viscosities, and temperatures; two distinct parts of the emission spectrum were selected for detection. Two prominent subnanosecond lifetimes in the fluorescence decays of the Cu(II) proteins could be observed. The decay of apo-azurin also consists of more than one component. The occurrence of more than one component in the fluorescence decays is explained by conformational heterogeneity. The anisotropy decay results appeared to be different for wild-type and mutated azurins. Phe110Ser and Ile7Ser azurin show more mobility of the Trp48 residue, as reflected in the order parameter.     

Probing the structure and mobility of Pseudomonas aeruginosa azurin by circular dichroism and dynamic fluorescence anisotropy.

The UV dynamic fluorescence and CD of several Pseudomonas aeruginosa azurins bearing single amino acid mutation have been studied. Two classes of mutants were examined. In the first class, two hydrophobic residues in the core of the protein, Ile 7 and Phe 110, nearest to the azurin single tryptophan Trp 48, were substituted by a serine (mutants 17S and F110S). In the second class, two residues in the outer sphere of the copper ligand field were changed, obtaining the following mutants: M44K, H35F, H35L, and H35Q. All these proteins showed two fluorescence lifetimes in the copper-containing form, but only one in the copper-free form. The lifetime of the latter derivatives was different from either those of the metal-bound samples, definitely ruling out the presence of apo-like species in the holo protein. Copper-free 17S and F110S showed a more complex fluorescence decay profile requiring a distribution of lifetimes rather than a single lifetime. Holo F110S was also better fitted, in the limit of confidence, with two distributions rather than a pair of lifetimes. Time-resolved anisotropy of these two mutants as well as of wild-type (wt) protein showed two components (rotational times for wt < or = 200 ps and 7 ns, respectively). These components were not affected significantly by copper removal in the case of wt protein. Instead, the short rotational component of the mutants dropped dramatically to values near zero, indicating a much greater mobility of the tryptophanyl residue in the mutant apo azurins. These data were supported by CD measurements showing a small effect of the copper presence in the region below 250 nm, i.e., in the secondary structure, but almost a collapse of the aromatic asymmetry at 270-295 nm related to a relaxation of the structural constraint around the tryptophan. Altogether these data show that copper does not play a structural role in wt azurin, whereas it is crucial in the stabilization of 17S and F110S mutants. Furthermore, although the metal site geometry is rigidly kept in wt apo-azurin, it regains the native form only in the presence of the metal in the "core" mutants. This finding is important for the theory of entatic states in metalloproteins (Williams RJP, 1995, Eur J Biochem 234:363-381).     

Time resolved spectroscgpy of tryptopkyl fluorescence of yeast 3-phosphoglycerate kinase

The tryptophyl fluorescence emission of yeast 3-phosphoglycerate kinase decreases from pH 3.9 to pH 7.2 following a normal titration curve with an apparent pK of 4.7. The fluorescence decays have been determined at both extreme pH by photocounting pulse fluorimetry and have been found to vary with the emission wavelength. A quantitative analysis of these results according to a previously described method allows to determine the emission characteristics of the two tryptophan residues present in the protein molecule. At pH 3.9, one of the tryptophan residues is responsible for only 13% of the total fluorescence emission. This first residue has a lifetime τ₁= 0.6 ns and a maximum fluorescence wavelength λ_2max = 332 nm. The second tryptophan residue exhibits two lifetimes τ₂₁= 3.1 ns and τ₂₂= 7.0 ns (λ_2max= 338 nm). In agreement with the attribution of τ₂₁and τ₃₂ to the same tryptophan residue, the ratio β = C₂₁/C₂₂ of the normalized amplitudes is constant along the fluorescence emission spectrum. At pH 7.2, the two tryptophan residues contribute almost equally tc the protein fluorescence. The decay time of tryptophan 1 is 0.4 ns. The other emission parameters are the same as those determined at pH 3.9. We conclude that the fluorescence quenching in the range pH 3.9 to pH 8.0 comes essentially from the formation of a non emitting internal ground state complex between the tryptophan having the longest decay times and a neighbouring protein chemical group. The intrinsic pK of this group and the equilibrium constant of the irternal complex can be estimated. The quenching group is thought to be a carboxylate anion. Excitation transfers between the two tryptophyl residues of the protein molecule appear to have a small efficiency.     

A time-resolved fluorescence study of azurin and metalloazurin derivatives

Nickel and cobalt derivatives of Pseudomonas fluorescens (ATCC 13525) azurin were prepared and their steady-state fluorescence and time-resolved fluorescence monitored. Like the copper-containing native protein, the fluorescence decay of both metallo derivatives was best fit to a sum of three exponentials, whereas the apoazurin from which they were prepared obeyed single-exponential decay kinetics. However, comparison of the lifetimes and fractional of each of the components in these derivatives to those in the oxidized and reduced native proteins revealed significant differences. These results suggest that the presence of a metal center in azurin imparts a conformational heterogeneity which is strongly dependent on the nature of the metal center. Further, the results are used to comment on current ideas concerning the geometry of the active site in this redox protein.     

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.     

Decay-associated fluorescence spectra and the heterogeneous emission of alcohol dehydrogenase

A procedure is described for using nanosecond time resolved fluorescence decay data to obtain decay-associated fluorescence spectra. It is demonstrated that the individual fluorescence spectra of two or more components in a mixture can be extracted without prior knowledge of their spectral shapes or degree of overlap. The procedure is also of value for eliminating scattered light artifacts in the fluorescence spectra of turbid samples. The method was used to separate the overlapping emission spectra of the two tryptophan residues in horse liver alcohol dehydrogenase. Formation of a ternary complex between the enzyme, NAD+, and pyrazole leads to a decrease in the total tryptophan fluorescence. It is shown that the emission of both tryptophan residues decreases. The buried tryptophan (residue 314) undergoes dynamic quenching with no change in the spectral distribution. Under the same conditions, the fluorescence intensity of tryptophan (residue 15) decreases without a change in decay time but with a red shift of the emission spectrum. There is also a decrease in tryptophan fluorescence intensity when the free enzyme is acid denatured (succinate buffer, pH 4.1). The denatured enzyme retains sufficient structure to provide different microenvironments for different tryptophan residues as reflected by biexponential decay and spectrally shifted emission spectra (revealed by decay association). The value of this technique for studies of microheterogeneity in biological macromolecules is discussed.     

Dynamics of tryptophan in the histidine-containing phosphocarrier protein of Streptomyces coelicolor: evidence of multistate equilibrium unfolding

The nanosecond dynamics of the single tryptophan, Trp10, of HPr from Streptomyces coelicolor, HPrsc, has been monitored at different pHs. Time-resolved fluorescence methods and DOSY measurements have been used to map the compactness of the protein. At low pHs, where a molten globule-like species has been described, the correlation times from fluorescence showed an abrupt change as the pH was increased. When the protein was folded (above pH 4), two correlation times were observed, which remained practically constant up to pH 9.5. The long correlation time, around 7.5 ns, corresponds to the global rotational motion of the protein, since this value is in agreement with that determined theoretically from hydrodynamic measurements. The short correlation time, around 1.4 ns, must report on fast movements of the protein segment containing the tryptophan residue. On the other hand, fluorescence lifetimes showed the same abrupt change as the correlation times at low pH, but, in addition, a sigmoidal change with a pKa approximately 4.3 was also observed. On the basis of the modeled structure of HPrsc, this last transition could be due to the proximity of Glu12 to Trp10. The changes monitored by the fluorescence lifetimes agree with those observed previously by steady-state fluorescence, CD, and ANS binding experiments. Taken together, these data suggest a multistate equilibrium during folding of HPrsc starting from low pHs.     

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.     

Investigation of the structural determinants of the intrinsic fluorescence emission of the trp repressor using single tryptophan mutants.

The fluorescence decay properties of wild-type trp repressor (TR) have been characterized by carrying out a multi-emission wavelength study of the frequency response profiles. The decay is best analyzed in terms of a single exponential decay near 0.5 ns and a distribution of lifetimes centered near 3-4 ns. By comparing the recovered decay associated spectra and lifetime values with the structure of the repressor, tentative assignments of the two decay components recovered from the analysis to the two tryptophan residues, W19 and W99, of the protein have been made. These assignments consist of linking the short, red emitting component to emission from W99 and most of the longer bluer emitting lifetime distribution to emission from W19. Next, single tryptophan mutants of the repressor in which one of each of the tryptophan residues was substituted by phenylalanine were used to confirm the preliminary assignments, inasmuch as the 0.5-ns component is clearly due to emission from tryptophan 99, and much of the decay responsible for the recovered distribution emanates from tryptophan 19. The data demonstrate, however, that the decay of the wild-type protein is not completely resolvable due both to the large number of components in the wild-type emission (at least five) as well as to the fact that three of the five lifetime components are very close in value. The fluorescence decay of the wild-type decay is well described as a combination of the components found in each of the mutants. However, whereas the linear combination analysis of the 15 data sets (5 from the wild-type and each mutant) yields a good fit for the components recovered previously for the two mutants, the amplitudes of these components in the wild-type are not recovered in the expected ratios. Because of the dominance of the blue shifted emission in the wild-type protein, it is most likely that subtle structural differences in the wild-type as compared with the mutants, rather than energy transfer from tryptophan 19 to 99, are responsible for this failure of the linear combination hypothesis.     

Photophysics of metalloazurins

The fluorescence lifetimes of Cu(II), Cu(I), Ag(I), Hg(II), Co(II), and Ni(II) azurin Pae from Pseudomonas aeruginosa and Cu(II), Cu(I), and Hg(II) azurin Afe from Alcaligenes faecalis were measured at 295 K by time-correlated single-photon counting. In addition, fluorescence lifetimes of Cu(II) azurin Pae were measured between 30 and 160 K and showed little change in value. Ultraviolet absorption difference spectra between metalloazurin Pae and apoazurin Pae were measured, as were the fluorescence spectra of metalloazurins. These spectra were used to determine the spectral overlap integral required for dipole-dipole resonance calculations. All metalloazurins exhibit a reduced fluorescence lifetime compared to their respective apoazurins. Forster electronic energy transfer rates were calculated for both metalloazurin Pae and metalloazurin Afe derivatives; both enzymes contain a single tryptophyl residue which is located in a different position in the two azurins. These azurins have markedly different fluorescence spectra, and electronic energy transfers occur from these two tryptophyl sites with different distances and orientations and spectral overlap integral values. Intramolecular distances and orientations were derived from an X-ray crystallographic structure and a molecular dynamic simulation of the homologous azurin Ade from Alcaligenes denitrificans, which contains both tryptophyl sites. Assignments were made of metal-ligand-field electronic transitions and of transition dipole moments and directions for tryptophyl residues, which accounted for the observed fluorescence quenching of Hg(II), Co(II), and Ni(II) azurin Pae and Cu(II) and Hg(II) azurin Afe. The fluorescence of azurin Pae is assigned as a 1Lb electronic transition, while that of azurin Afe is 1La. The marked fluorescence quenching of Cu(II) azurin Pae and Cu(I) azurin Pae and Afe is less well reproduced by our calculations, and long-range oxidative and reductive electron transfer, respectively, are proposed as additional quenching mechanisms. This study illustrates the application of Forster electronic energy transfer calculations to intramolecular transfers in structurally well characterized molecular systems and demonstrates its ability to predict observed fluorescence quenching rates when the necessary extensive structural, electronic transition assignment, and spectroscopic data are available. The agreement between Forster calculations and quenching rates derived from fluorescence lifetime measurements suggests there are limited changes in conformation between crystal structure and solution structures, with the exception of the tryptophyl residue of azurin Afe, where a conformation derived from a molecular simulation in water was necessary rather than that found in the crystal structure.     

Analysis of time-resolved fluorescence anisotropy in lipid-protein systems

The subnanosecond fluorescence and motional dynamics of the tryptophan residue in the bacteriophage M13 coat protein incorporated within pure dioleoylphosphatidylcholine (DOPC) as well as dioleoylphosphatidylcholine/dioleoylphosphatidylglycerol (DOPC/DOPG) and dimyristoylphosphatidylcholine/dimyristoylphosphatidylglycerol (DMPC/DMPG) bilayers (80/20 w/w) with various L/P ratio have been investigated. The fluorescence decay is decomposed into four components with lifetimes of about 0.5, 2.0, 4.5 and 10.0 ns, respectively. In pure DOPC and DOPC/DOPG lipid bilayers, above the phase transition temperature, the rotational diffusion of the protein molecules contributes to the depolarization and the anisotropy of tryptophan is fitted to a dual exponential function. The longer correlation time, describing the rotational diffusion of the whole protein, shortens with increasing temperature and decreasing protein aggregation number. In DMPC/DMPG lipid bilayers, below the phase transition, the rotational diffusion of the protein is slowed down such that the subnanosecond anisotropy decay of tryptophan in this system reflects only the segmental motion of the tryptophan residue. Because of a heterogeneous microenvironment, the anisotropy decay must be described by three exponentials with a constant term, containing a negative coefficient and a negative decay time constant. From such a decay, the tryptophan residue within the aggregate undergoes a more restricted motion than the one exposed to the lipids. At 20 degrees C, the order parameter of the transition moment of the isolated tryptophan is about 0.9 and that for the exposed one is about 0.5.     

A time-resolved fluorescence study of human copper-zinc superoxide dismutase

The intrinsic fluorescence decay of human Cu,Zn superoxide dismutase was measured by frequency-domain techniques. The protein consists of two subunits, each containing one tryptophan and no tyrosine residues. Using a synchrotron radiation source, which allows facile selection of the excitation wavelength, the dependence of the emission decay upon excitation was studied. No significant excitation wavelength effects were found. The two tryptophans contained in the dimer, although fully equivalent and exposed to solvent, showed a fluorescence decay that cannot be described by a single lifetime. Either two lifetimes, or one Lorentzian-shaped continuous distribution of lifetimes, are needed to obtain a good fit. Under identical experimental conditions, control experiments showed that N-acetyltryptophanamide, an analogue of tryptophanyl residues in proteins, decays with a single lifetime. The heterogeneous decay of tryptophan fluorescence in superoxide dismutase is interpreted as due to the presence of static and/or dynamic conformers in the protein that decay with different lifetimes. The two models of discrete lifetimes and continuous distribution of lifetimes are discussed with reference to measurements on holo- and apo-human superoxide dismutase.     

Interaction of influenza hemagglutinin amino-terminal peptide with phospholipid vesicles: a fluorescence study

We have studied tryptophan fluorescence from a 20-residue synthetic peptide corresponding to the amino terminal of the HA2 subunit of the influenza virus hemagglutinin protein, a putative "fusion" peptide. Decay-associated spectra have been obtained at pH 7.4 and at pH 5 (the optimal pH for influenza virus fusion) in the presence and absence of liposomes. We demonstrate that a blue shift in the total steady-state fluorescence spectrum upon binding to liposomes is due to a movement in characteristic emission wavelength and increased lifetime of one of the resolved spectral components. In contrast, a further shift after lowering the pH is the product of a redistribution in the relative amplitudes of spectral components. Also, each decay component is quenched by spin-labels or anthroxyl groups normally located within the hydrocarbon interior of the membranes. Calculations are presented leading to an estimate of the distance of the tryptophan residue from the bilayer center, suggesting that the tryptophan residues are at or near the hydrocarbon-polar interface. No gross positional change was detected between pH values. Rotational depolarization is shown to be retarded by liposome binding, more so at low pH.     

Photophysics of tryptophan in bacteriophage T4 lysozymes

Bacteriophage T4 lysozyme contains three tryptophan residues in distinct environments. Lysozymes with one or two of these residues replaced by tyrosine are used to characterize the photophysics of tryptophan in these individual sites. The fluorescence spectra, average lifetimes, and quantum yields of these three single-tryptophan variants are understandable in terms of the neighboring residues. The emission spectra and radiative lifetimes are found to be the same for all three species while the quantum yield and decay kinetics are quite distinct. The variation of the average nonradiative rate constant is correlated with neighboring quenching groups. Quenching by I- correlates with exposure of the tryptophan residue based on the crystal structure. Complex behavior is observed for the time dependence of the fluorescence decay in all three cases, including that of the immobile tryptophan-138 residue. The complexity of the fluorescence decay is ascribed to heterogeneity in the nonradiative rate constant among microstates. Energy transfer between tryptophan residues is inferred to occur from comparison of the quantum yields of the two-tryptophan and single-tryptophan proteins and is discussed in terms of the F?rster mechanism.     

Fluorescence dynamics of staphylococcal nuclease in aqueous solution and reversed micelles

The dynamical fluorescence properties of the sole tryptophan residue (Trp-140) in Staphylococcus aureus nuclease (EC 3.1.31.1) have been investigated in aqueous solution and reversed micelles composed of either sodium bis(2-ethylhexyl)sulfosuccinate (AOT) in isooctane or cetyltrimethylammonium chloride (CTAC) in isooctane/hexanol (12:1 by volume). The fluorescence decay of nuclease in the different environments can be described by a trimodal distribution of fluorescence lifetimes at approx. 0.5, 1.5 and 5.0 ns. The relative amplitudes depend on the environment. For pH 9.0 solutions the contribution of the two shortest lifetime components in the distribution is largest for AOT and smallest for CTAC reversed micelles. There is reasonable agreement between the average fluorescence lifetime and the fluorescence quantum efficiency confirming a significant fluorescence quenching in AOT reversed micelles. Fluorescence anisotropy decay revealed that the tryptophan environment in aqueous nuclease solutions is rigid on a nanosecond timescale. When nuclease was entrapped into reversed micelles the tryptophan gained some internal flexibility as judged from the distinct presence of a shorter correlation time. The longer correlation time reflected the rotational properties of the protein-micellar system. Modulation of the overall charge of nuclease (isoelectric point pH 9.6) by using buffer of pH 9.0 and pH 10.4, respectively, and of the size of empty micelles by selecting two values of the water to surfactant molar ratio, had only a minor effect on the rotational properties of nuclease in the positively charged reversed micelles. Encapsulation of nuclease in anionic reversed micelles resulted in the development of protein bound to aggregated structures which are immobilised on a nanosecond timescale. According to far UV vircular dichroism results the secondary structure of nuclease only followed the already published pH-dependent changes. Encapsulation had no major effect on the overall secondary structure.