A step toward the prediction of the fluorescence lifetimes of tryptophan residues in proteins based on structural and spectral data

A method is presented that allows the calculation of the lifetimes of tryptophan residues on the basis of spectral and structural data. It is applied to two different proteins. The calcium binding protein from the sarcoplasm of the muscles of the sand worm Nereis diversicolor (NSCP) changes its conformation upon binding of Ca2+ or Mg2+. NSCP contains three tryptophan residues at position 4, 57, and 170, respectively. The fluorescence lifetimes of W57 are investigated in a mutant in which W4 and W170 have been replaced. The time resolved fluorescence properties of W57 are linked to its different microconformations, which were determined by a molecular dynamics simulation map. Together with the determination of the radiative rate constant from the wavelength of maximum intensity of the decay associated spectra, it was possible to determine an exponential relation between the nonradiative rate constant and the distance between the indole CE3 atom and the carbonyl carbon of the peptide bond reflecting a mechanism of electron transfer as the main determinant of the value for the nonradiative rate constant. This result allows the calculation of the fluorescence lifetimes from the protein structure and the spectra. This method was further tested for the tryptophan of Ha-ras p21 (W32) and for W43 of the Tet repressor, which resulted in acceptable values for the predicted lifetimes.     

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.     

Tryptophan properties in fluorescence and functional stability of plasminogen activator inhibitor 1

Plasminogen activator inhibitor 1 harbors four tryptophan residues at positions 86, 139, 175, and 262. To investigate the contribution of each tryptophan residue to the total fluorescence and to reveal the mutual interactions of the tryptophan residues and interactions with the other amino acids, 15 mutants in which tryptophan residues have been replaced by phenylalanines were constructed, purified, and characterized. Conformational distribution analysis revealed that the tryptophan mutants have a similar conformational distribution pattern as wild-type plasminogen activator inhibitor 1. Mutants in which tryptophan residue 175 was replaced by a phenylalanine displayed an increased functional half-life of the active conformation, whereas the functional half-life of mutants in which tryptophan residue 262 was replaced by a phenylalanine was substantially decreased. Comparative analysis of the fluorescence lifetimes, the extinction coefficients, and the quantum yields of the individual tryptophan residues demonstrates that tryptophan residue 262 gives the highest contribution to the total fluorescence. The other tryptophan residues have a very low quantum yield. In the wild-type protein, the fluorescence of all tryptophan residues is partially quenched as compared to the mutants that contain single tryptophan residues, due to conformational effects. The fluorescence of tryptophan residue 262 is very likely also partially quenched by energy transfer to tryptophan residue 175.     

Time-resolved fluorescence study of the single tryptophans of engineered skeletal muscle troponin C.

The regulatory domain of troponin C (TnC) from chicken skeletal muscle was studied using genetically generated mutants which contained a single tryptophan at positions 22, 52, and 90. The quantum yields of Trp-22 are 0.33 and 0.25 in the presence of Mg2+ (2-Mg state) and Ca2+ (4-Ca state), respectively. The large quantum yield of the 2-Mg state is due to a relatively small nonradiative decay rate and consistent with the emission peak at 331 nm. The intensity decay of this state is monoexponential with a single lifetime of 5.65 ns, independent of wavelength. In the 4-Ca state, the decay is biexponential with the mean of the two lifetimes increasing from 4.54 to 4.92 ns across the emission band. The decay-associated spectrum of the short lifetime is red-shifted by 19 nm relative to the steady-state spectrum. The decay of Trp-52 is biexponential in the 2-Mg state and triexponential in the 4-Ca state. The decay of Trp-90 requires three exponential terms for a satisfactory fit, but can be fitted with two exponential terms in the 4-Ca state. The lower quantum yields (< 0.15) of these two tryptophans are due to a combination of smaller radiative and larger nonradiative decay rates. The results from Trp-22 suggest a homogeneous ground-state indole ring in the absence of bound Ca2+ at the regulatory sites and a ground-state heterogeneity induced by activator Ca2+. The Ca(2+)-induced environmental changes of Trp-52 and Trp-90 deviate from those predicted by a modeled structure of the 4-Ca state. The anisotropy decays of all three tryptophans show two rotational correlation times. The long correlation times (phi 1 = 8.1-8.3 ns) derived from Trp-22 and Trp-90 suggest an asymmetric hydrodynamic shape. TnC becomes more asymmetric upon binding activator Ca2+ (phi 1 = 10.1-11.6 ns). The values of phi 1 obtained from Trp-52 are 3-4 ns shorter than those from Trp-22 and Trp-90, and these reduced correlation times may be related to the mobility of the residue and/or local segmental flexibility.     

Time-resolved fluorescence and anisotropy decay of the tryptophan in adrenocorticotropin-(1-24)

The direct time-resolved fluorescence anisotropy of the single tryptophan residue in the polypeptide hormone adrenocorticotropin-(1-24) (ACTH) and the fluorescence decay kinetics of this residue (Trp-9) are reported. Two rotational correlation times are observed. One, occurring on the subnanosecond time scale, reflects the rotation of the indole ring, and the other, which extends into the nanosecond range, is dominated by the complex motions of the polypeptide chain. The fluorescence lifetimes of the single tryptophan in glucagon (Trp-25) and the 23-26 glucagon peptide were also measured. In all cases the fluorescence kinetics were satisfied by a double-exponential decay law. The fluorescence lifetimes of several tryptophan and indole derivatives and two tryptophan dipeptides were examined in order to interpret the kinetics. In close agreement with the findings of Szabo and Rayner [Szabo, A. G., & Rayner, D. M. (1980) J. Am. Chem. Soc. 102, 554-563], the tryptophan zwitterion exhibits emission wavelength dependent double-exponential decay kinetics. At 320 nm tau 1 = 3.2 ns and tau 2 = 0.8 ns, with alpha 1 = 0.7 and alpha 2 = 0.3. Above 380 nm only the 3.2-ns component is observed. By contrast the neutral derivative N-acetyltryptophanamide has a single exponential decay of 3.0 ns. The multiexponential decay kinetics of the polypeptides are discussed in terms of flexibility of the polypeptide chain and neighboring side-chain interactions.     

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.     

The dead-end elimination method,tryptophan rotamers,and fluorescence lifetimes

The Dead-End Elimination method was used to identify 40 low energy microconformations of 16 tryptophan residues in eight proteins. Single Trp-mutants of these proteins all show a double- or triple-exponential fluorescence decay. For ten of these lifetimes the corresponding rotameric state could be identified by comparing the bimolecular acrylamide quenching constant (k(q)) and the relative solvent exposure of the side chain in that microstate. In the absence of any identifiable quencher, the origin of the lifetime heterogeneity is interpreted in terms of the electron transfer process from the indole C epsilon 3 atom to the carbonyl carbon of the peptide bond. Therefore it is expected that a shorter [C epsilon 3-C[double bond]O] distance leads to a shorter lifetime as observed for these ten rotamers. Applying the same rule to the other 30 lifetimes, a link with their corresponding rotameric state could also be made. In agreement with the theory of Marcus and Sutin, the nonradiative rate constant shows an exponential relationship with the [C epsilon 3-C[double bond]O] distance for the 40 datapoints.     

Resolution of the fluorescence decay of the two tryptophan residues of lac repressor using single tryptophan mutants.

We have studied the time-resolved intrinsic tryptophan fluorescence of the lac repressor (a symmetric tetramer containing two tryptophan residues per monomer) and two single-tryptophan mutant repressors obtained by site-directed mutagenesis, lac W201Y and lac W220Y. These mutant repressor proteins have tyrosine substituted for tryptophan at positions 201 and 220, respectively, leaving a single tryptophan residue per monomeric subunit at position 220 for the W201Y mutant and at position 201 in the W220Y mutant. It was found that the two decay rates recovered from the analysis of the wild type data do not correspond to the rates recovered from the analysis of the decays of the mutant proteins. Each of these residues in the mutant repressors displays at least two decay rates. Global analysis of the multiwavelength data from all three proteins, however, yielded results consistent with the fluorescence decay of the wild type lac repressor corresponding simply to the weighted linear combination of the decays from the mutant proteins. The effect of ligation by the antagonistic ligands, inducer and operator DNA, was similar for all three proteins. The binding of the inducer sugar resulted in a quenching of the long-lived species, while binding by the operator decreased the lifetime of the short components. Investigation of the time-resolved anisotropy of the intrinsic tryptophan fluorescence in these three proteins revealed that the depolarization of fluorescence resulted from a fast motion and the global tumbling of the macromolecule. Results from the simultaneous global analysis of the frequency domain data sets from the three proteins revealed anisotropic rotations for the macromolecule, consistent with the known elongated shape of the repressor tetramer. In addition, it appears that the excited-state dipole of tryptophan 220 is alighed with the long axis of the repressor.     

Study of the time-resolved tryptophan fluorescence of crystalline alpha-chymotrypsin

The tryptophan environments in crystalline alpha-chymotrypsin were investigated by fluorescence. The heterogeneous emission from this multitryptophan enzyme was resolved by time-correlated fluorescence spectroscopy. The fluorescence decays at 296-nm laser excitation and various emission wavelengths could be characterized by a triple-exponential function with decay times tau 1 = 150 +/- 50 ps, tau 2 = 1.45 +/- 0.25 ns, and tau 3 = 4.2 +/- 0.4 ns. The corresponding decay-associated emission spectra of the three components had maxima at about 325, 332, and 343 nm. The three decay components in this enzyme can be correlated with X-ray crystallographic data [Birktoft, J.J., & Blow, D.M. (1972) J. Mol. Biol. 68, 187-240]. Inter- and intramolecular tryptophan-tryptophan energy-transfer efficiencies in crystalline alpha-chymotrypsin were computed from the accurately known positions and orientations of all tryptophan residues. These calculations indicate that the three fluorescence decay components in crystalline alpha-chymotrypsin can be assigned to three distinct classes of tryptophyl residues. Because of the different proximity of tryptophan residues to neighboring internal quenching groups, the decay times of the three classes are different. Decay tau 1 can be assigned to Trp-172 and Trp-215 and tau 2 to Trp-51 and Trp-237, while the tryptophyl residues 27, 29, 141, and 207 all have decay time tau 3.     

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.     

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.     

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.     

Fluorescence of tryptophan dipeptides: correlations with the rotamer model

The multiexponential decay of tryptophan derivatives has previously been explained by the presence of rotamers having different fluorescence lifetimes, but it has been difficult to correlate rotamer structure and physical properties. New time-resolved and static data on dipeptides of the type Trp-X and X-Trp, where X is another aminoacyl residue, are consistent with the rotamer model and allow some correlations. That a dominant rotamer of Trp-X zwitterion has the -NH3+ group near the indole ring was inferred from absorption and fluorescence spectra, titrimetric determination of pKa values, photochemical hydrogen-deuterium-exchange experiments, decay-associated spectra, quantum yields, and decay kinetics. Analysis of the lifetime and quantum yield data for Trp dipeptides, especially X-Trp, suggests that static self-quenching is not uncommon. Highly quenched and weak components of the fluorescence do not contribute to the calculated mean lifetime, thus resulting in apparent static quenching. We propose the term quasi-static self-quenching (QSSQ) to distinguish this phenomenon from quenching due to ground-state formation of a dark complex. Mechanisms of quenching and the structure of statically quenched rotamers are discussed. The occurrence of QSSQ supports the idea that rotamers interconvert slowly. A major perceived deficiency of the rotamer model, namely, the apparent inability to predict reasonable rotamer populations from fluorescence decay data, may result from the presence of statically quenched species, which do not contribute to the fluorescence.     

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.     

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.     

Comparative structural analysis of staphylococcal enterotoxins A and E

Structural analysis of staphylococcal enterotoxins A and E, two functionally and serologically related proteins, has been carried out using circular dichroism, and tryptophan fluorescence quantum yield and quenching. Secondary structures derived from the far-UV circular dichroic spectra revealed that both enterotoxins are in predominantly beta-sheets/beta-turn structures (80-85%). Staphylococcal enterotoxin A has significantly higher alpha-helical content (10.0%) than staphylococcal enterotoxin E (6.5%). Tryptophan fluorescence spectra of both enterotoxins showed maxima at approximately 342 nm, indicating that the fluorescent tryptophan residues are in polar environments. However, the tryptophan fluorescence quantum yields indicated that tryptophan residues are approximately 41% more fluorescent in staphylococcal enterotoxin A than in staphylococcal enterotoxin E. Tryptophan fluorescence quenching by a surface quencher, I-, and a neutral quencher, acrylamide, indicated that at least 1 of the 2 tryptophan residues in both staphylococcal enterotoxins A and E is located on the outer surface of the proteins. This tryptophan residue is in significantly different environments in the two enterotoxins. Six antigenic sites are predicted from the hydrophilicity and secondary structure information; at least four sites are identical. In general, staphylococcal enterotoxins A and E have some structural similarities which are compatible with their common biological activities.     

Ferredoxin from Halobacterium of the Dead Sea. Structural properties revealed by fluorescence techniques

The two tryptophan residues of ferredoxin from Halobacterium of the Dead Sea differ in their fluorescence characteristics. One of these tryptophan residues (class 1) absorbs more to the red and is thus probably in a more apolar environment than the other (class 2). Upon removal of the ferric ions, i.e., in the apoferredoxin, a 2.2-fold increase in the quantum yield of fluorescence is observed. A double exponential decay of the fluorescence is found for ferredoxin, reduced ferredoxin, as well as for the apoferredoxin. The longer decay time assumes a constant value of 6.9 ns in all three cases, indicating that it originates in a tryptophan residue which is not affected by changes in the Fe³⁺ binding site (class 2 tryptophan). The shorter decay component increases gradually from 0.55 ns in oxidized ferredoxin, through 0.80 ns in the reduced ferredoxin to 1.24 ns in the apoprotein. This decay component is thus assumed to be largely due to the second tryptophan residue of the protein (class 1) located close to the Fe³⁺ binding site. On the other hand, the relative decay amplitude of the class 2 tryptophan is doubled upon formation of apoferredoxin. It is concluded that the class 1 tryptophan is quenched by the active site ferric ions and that the class 2 tryptophan is partially exposed to a polar environment. Whereas class 1 tryptophan may be similar to the single nonfluorescent tryptophan of spinach ferredoxin, class 2 tryptophan is found in a peptide which is present only in halophilic ferredoxins. Conformational changes occur in the molecule upon removal—but not reduction—of the ferric ions, causing the environment of the class 2 tryptophan to become more hydrophobic. It is possible that the class 1 tryptophan is associated with the occurrence of a higher redox potential in this ferredoxin, when compared with chloroplast-type ferredoxins.     

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.     

Excited‐state lifetime studies of the three tryptophan residues in the N‐lobe of human serum transferrin

The energy transfer from the three Trp residues at positions 8, 128, and 264 within the human serum transferrin (hTF) N-lobe to the ligand to metal charge transfer band has been investigated by monitoring changes in Trp fluorescence emission and lifetimes. The fluorescence emission from hTF N-lobe is dominated by Trp264, as revealed by an 82% decrease in the quantum yield when this Trp residue is absent. Fluorescence lifetimes were determined by multifrequency phase fluorometry of mutants containing one or two Trp residues. Decays of these samples are best described by two or three discrete lifetimes or by a unimodal Lorentzian distribution. The discrete lifetimes and the center of the lifetime distribution for samples containing Trp128 and Trp264 are affected by iron. The distribution width narrows on iron removal and is consistent with a decrease in dynamic mobility of the dominant fluorophore, Trp264. Both the quantum yield and the lifetimes are lower when iron is present, however, not proportionally. The greater effect of iron on quantum yields is indicative of nonexcited state quenching, i.e., static quenching. The results of these experiments provide quantitative data strongly suggesting that Förster resonance energy transfer is not the sole source of Trp quenching in the N-lobe of hTF.