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.     

Determination of the excited-state lifetimes of the tryptophan residues in barnase, via multifrequency phase fluorometry of tryptophan mutants.

A multifrequency phase fluorometric study is described for wild-type barnase and engineered mutant proteins in which tryptophan residues have been replaced by less fluorescent residues which do not interfere with the determination of the tryptophan emission spectra and lifetimes. The lifetimes of the three tryptophans in the wild-type protein have been resolved. Trp-35 has a single fluorescence lifetime, which varies in the different proteins between 4.3 and 4.8 ns and is pH-independent between pH 5.8 and 8.9. Trp-71 and Trp-94 behave as an energy-transfer couple with both forward and reverse energy transfer. The couple shows two fluorescence lifetimes: 2.42 (+/-0.2) and 0.74 (+/-0.1) ns at pH 8.9, and 0.89 (+/-0.05) and 0.65 (+/-0.05) ns at pH 5.8. In the mutant Trp-94----Phe the lifetime of Trp-71 is 4.73 (+/-0.008) ns at high pH and 4.70 (+/-0.004) ns at low pH. In the mutant Trp-71----Tyr, the lifetime of Trp-94 is 1.57 (+/-0.01) ns at high pH and 0.82 (+/-0.025) ns at low pH. From these lifetimes, one-way energy-transfer efficiencies can be calculated according to Porter [Porter, G.B. (1972) Theor. Chim. Acta 24, 265-270]. At pH 8.9, a 71% efficiency was found for forward transfer (from Trp-71 to Trp-94) and 36% for reverse transfer. At pH 5.8 the transfer efficiency was 86% for forward and 4% for reverse transfer (all +/-2%). These transfer efficiencies correspond fairly well with the ones calculated according to the theory of F?rster [F?rster, T. (1948) Ann. Phys. (Leipzig) 2, 55-75].(ABSTRACT TRUNCATED AT 250 WORDS)     

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.     

Picosecond-resolved fluorescence spectra of D-amino-acid oxidase. A new fluorescent species of the coenzyme

Protein dynamics of D-amino-acid oxidase in the picosecond region was investigated by measuring time-resolved fluorescence of the bound coenzyme, FAD. The observed nonexponential fluorescence decay curves were analyzed with four-exponential decay functions. The fluorescence lifetimes at the best fit were 26.6 +/- 0.7 ps, 44.0 +/- 4.2 ps, 177 +/- 11 ps, and 2.28 +/- 0.21 ns at 20 degrees C and 25.2 +/- 3.0 ps, 50.3 +/- 8.7 ps, 228 +/- 27 ps, and 2.75 +/- 0.33 ns at 5 degrees C. Component fractions with the shortest lifetime, ca. 26 ps, were always negative and close to -1. The other fluorescent components of the lifetimes, ca. 47 ps, 200 ps, and 2.6 ns, with positive fractions were assigned to different forms of the enzyme including the dimer, the monomer, and free FAD dissociated from the enzyme. Measurements of the time-resolved fluorescence spectra revealed that the maximum wavelengths of the spectra shifted toward shorter wavelength by 65 nm at 20 degrees C and 36 nm at 5 degrees C within 100 ps after pulsed excitation. The remarkable blue shift was not observed in free FAD. The first spectra immediately after the excitation of the enzyme exhibited maximum wavelengths of 584 nm at 20 degrees C and 557 nm at 5 degrees C. The fluorescence spectra obtained at times later than 100 ps are in good agreement with the one obtained under steady-state excitation of D-amino-acid oxidase.(ABSTRACT TRUNCATED AT 250 WORDS)     

One- and two-photon excited fluorescence lifetimes and anisotropy decays of green fluorescent proteins

We have used one- (OPE) and two-photon (TPE) excitation with time-correlated single-photon counting techniques to determine time-resolved fluorescence intensity and anisotropy decays of the wild-type Green Fluorescent Protein (GFP) and two red-shifted mutants, S65T-GFP and RSGFP. WT-GFP and S65T-GFP exhibited a predominant approximately 3 ns monoexponential fluorescence decay, whereas for RSGFP the main lifetimes were approximately 1.1 ns (main component) and approximately 3.3 ns. The anisotropy decay of WT-GFP and S65T-GFP was also monoexponential (global rotational correlation time of 16 +/- 1 ns). The approximately 1.1 ns lifetime of RSGFP was associated with a faster rotational depolarization, evaluated as an additional approximately 13 ns component. This feature we attribute tentatively to a greater rotational freedom of the anionic chromophore. With OPE, the initial anisotropy was close to the theoretical limit of 0.4; with TPE it was higher, approaching the TPE theoretical limit of 0.57 for the colinear case. The measured power dependence of the fluorescence signals provided direct evidence for TPE. The general independence of fluorescence decay times, rotation correlation times, and steady-state emission spectra on the excitation mode indicates that the fluorescence originated from the same distinct excited singlet states (A*, I*, B*). However, we observed a relative enhancement of blue fluorescence peaked at approximately 440 nm for TPE compared to OPE, indicating different relative excitation efficiencies. We infer that the two lifetimes of RSGFP represent the deactivation of two substates of the deprotonated intermediate (I*), distinguished by their origin (i.e., from A* or B*) and by nonradiative decay rates reflecting different internal environments of the excited-state chromophore.     

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.     

Protein structural requirements and properties of membrane binding by gamma-carboxyglutamic acid-containing plasma proteins and peptides

The membrane-binding characteristics of a number of modified vitamin K-dependent proteins and peptides showed a general pattern of structural requirements. The amino-terminal peptides from human prothrombin (residues 1-41 and 1-44, 60:40) bovine factor X (residues 1-44), and bovine factor IX (residues 1-42), showed a general requirement for a free amino-terminal group, an intact disulfide, and the tyrosine homologous to Tyr44 of factor X for membrane binding. Consequently, the peptide from factor IX did not bind to membranes. Any of several modifications of the amino terminus, except reaction with trinitrobenzenesulfonic acid, abolished membrane binding by the factor X and prothrombin peptides. Calcium, but not magnesium, protected the amino terminus from chemical modification. The requirement for a free amino terminus was also shown to be true for intact prothrombin fragment 1, factor X, and factor IX. Although aggregation of the peptide-vesicle complexes greatly complicated accurate estimation of equilibrium binding constants, results with the factor X peptide indicated an affinity that was not greatly different from that of the parent protein. The most striking difference shown by the peptides was a requirement for about 10 times as much calcium as the parent proteins. In a manner similar to the parent proteins, the prothrombin and factor X peptides showed a large calcium-dependent quenching of tryptophan fluorescence. This fluorescence quenching in the peptides also required about 10 times the calcium needed by the parent proteins. Thus, the 1-45 region of the vitamin K-dependent proteins contained most of the membrane-binding structure but lacked component(s) needed for high affinity calcium binding. Protein S that was modified by thrombin cleavage at Arg52 and Arg70 showed approximately the same behavior as the amino-terminal 45-residue peptides. That is, it bound to membranes with overall affinity that was similar to native protein S but required high calcium concentrations. These results suggested that the second disulfide loop of protein S (Cys47-Cys72) and prothrombin (Cys48-Cys61) were involved in high affinity calcium binding. Since factor X lacks a homologous disulfide loop, an alternative structure must serve a similar function. A striking property of protein S was dissociation from membranes by high calcium. While this property was shared by all the vitamin K-dependent proteins, protein S showed this most dramatically and supported protein-membrane binding by calcium bridging.     

Picosecond fluorescence of cryptomonad biliproteins. Effects of excitation intensity and the fluorescence decay times of phycocyanin 612, phycocyanin 645, and phycoerythrin 545.

The fluorescence of purified biliproteins (phycocyanin 645, phycocyanin 612, and phycoerythrin 545) from three cryptomonads, Chroomonas species, Hemiselmis virescens, and Rhodomonas lens, and C-phycocyanin from Anacystis nidulans has been time resolved in the picosecond region with a streak camera system having less than or equal to 2-ps jitter. The fluorescence lifetimes of phycocyanins from Chroomonas species and Hemiselmis virescens are 1.5 +/- 0.2 ns and 2.3 +/- 0.2 ns, respectively, regardless of the fluence of the 30 ps, 532-nm excitation pulse. (Fluence [or photons/cm2] = f intensity [photons/cm2s]dt.). In contrast, that of C-phycocyanin is 2.3 +/- 0.2 ns when the excitation fluence is 8.2 X 10(11) photons/cm2 and decreases to a decay approximated by an exponential decay time of 0.65 +/- 0.1 ns at 7.2 X 10(16) photons/cm2. The cryptomonad phycoerythrin fluorescence decay lifetime is also dependent on intensity, having a decay time of 1.5 +/- 0.1 ns at low fluences and becoming clearly biphasic at higher fluences (greater than 10(15) photons/cm2). We interpret the shortening of decay times for C-phycocyanin and phycoerythrin 545 in terms of exciton annihilation, and have discussed the applicability of exciton annihilation theories to the high fluence effects.     

Conformational effects on tryptophan fluorescence in cyclic hexapeptides

The peptide bond quenches tryptophan fluorescence by excited-state electron transfer, which probably accounts for most of the variation in fluorescence intensity of peptides and proteins. A series of seven peptides was designed with a single tryptophan, identical amino acid composition, and peptide bond as the only known quenching group. The solution structure and side-chain chi(1) rotamer populations of the peptides were determined by one-dimensional and two-dimensional (1)H-NMR. All peptides have a single backbone conformation. The -, psi-angles and chi(1) rotamer populations of tryptophan vary with position in the sequence. The peptides have fluorescence emission maxima of 350-355 nm, quantum yields of 0.04-0.24, and triple exponential fluorescence decays with lifetimes of 4.4-6.6, 1.4-3.2, and 0.2-1.0 ns at 5 degrees C. Lifetimes were correlated with ground-state conformers in six peptides by assigning the major lifetime component to the major NMR-determined chi(1) rotamer. In five peptides the chi(1) = -60 degrees rotamer of tryptophan has lifetimes of 2.7-5.5 ns, depending on local backbone conformation. In one peptide the chi(1) = 180 degrees rotamer has a 0.5-ns lifetime. This series of small peptides vividly demonstrates the dominant role of peptide bond quenching in tryptophan fluorescence.     

Calcium affinity of regulatory sites in skeletal troponin-C is attenuated by N-cap mutations of helix C

Site-directed mutagenesis was used to make amino acid substitutions at position 54 of skeletal troponin C, testing a relationship between the stability of helix C and calcium ion affinity at regulatory sites in the protein. Normally, threonine at position 54 is the first helical residue, or N-cap, of the C helix; where helices C and D, and the loop between, comprise binding site II. Mutations were made in the context of a previously described phenylalanine 29--> tryptophan (F29W) variant (Trigo-Gonzalez et al., Biochemistry 31, 7009-7015 (1992)), which allows binding events to be monitored through changes in the intrinsic fluorescence of the protein. N-Cap substitutions at position 54 were shown to attenuate the calcium affinity of regulatory sites in the N-terminal domain. Calcium affinities diminished according to the series T54 T54S > T54A > T54V > T54G with dissociation constants of 1.36 x 10(-6), 1.36 x 10(-6), 2.09 x 10(-6), 2.28 x 10(-6), and 4.24 x 10(-6) M, respectively. The steady state binding of calcium to proteins in the mutant series was seen to be monophasic and cooperative. Calcium off-rates were measured by stopped flow fluorescence and in every instance two transitions were observed. The rate constant of the first transition, corresponding to approximately 99% of the change in fluorescence, was between 900+/-20 and 1470+/-100 s(-1), whereas the rate constant of the second transitions was between 94+/-9 and 130+/-23 s(-1). The significance of two transitions remains unclear, though both rate constants occur on a time scale consistent with the regulation of contraction.     

Resolution of the lifetimes and correlation times of the intrinsic tryptophan fluorescence of human hemoglobin solutions using 2 GHz frequency-domain fluorometry

We used 2 GHz harmonic content frequency-domain fluorescence to measure the intensity and the anisotropy decays from the intrinsic tryptophan fluorescence from human hemoglobin (Hb). The tryptophan intensity decays are dominated by a short-lived component which accounts for 35-60% of the total steady state intensity. The decay time of this short component varies from 9 to 27 ps and this component is sensitive to the ligation state of Hb. Our error analyses indicate the uncertainty is about +/- 3 ps. The intensity decays also show two longer lived components near 0.7 and 8 ns, which are probably due either to impurities or to Hb molecules in conformations which do not permit energy transfer. The anisotropy decays indicate the tryptophan residues in Hb are highly mobile, with apparent correlation times near 55 ps.     

Time-resolved fluorescence of the single tryptophan of Bacillus stearothermophilus phosphofructokinase.

The fluorescence of the single tryptophan in Bacillus stearothermophilus phosphofructokinase was characterized by steady-state and time-resolved techniques. The enzyme is a tetramer of identical subunits, which undergo a concerted allosteric transition. Time-resolved emission spectral data were fitted to discrete and distributed lifetime models. The fluorescence decay is a double exponential with lifetimes of 1.6 and 4.4 ns and relative amplitudes of 40 and 60%. The emission spectra of both components are identical with maxima at 327 nm. The quantum yield is 0.31 +/- 0.01. The shorter lifetime is independent of temperature; the longer lifetime has weak temperature dependence with activation energy of 1 kcal/mol. The fluorescence intensity and decay are the same in H2O and D2O solutions, indicating that the indole ring is not accessible to bulk aqueous solution. The fluorescence is not quenched significantly by iodide, but it is quenched by acrylamide with bimolecular rate constant of 5 x 10(8) M-1 s-1. Static and dynamic light scattering measurements show that the enzyme is a tetramer in solution with hydrodynamic radius of 40 A. Steady-state and time-resolved fluorescence anisotropies indicate that the tryptophan is immobile. The allosteric transition has little effect on the fluorescence properties. The fluorescence results are related to the x-ray structure.     

Tryptophan interactions of gramicidin A′ channels in lipids: a time-resolved fluorescence study

The evolution of the incorporation of cation transport channels into lysolecithin micelles by gramicidin A was followed by measuring the ns time-resolved fluorescence of the tryptophan residues. In all samples, the tryptophan fluorescence could be resolved into three exponentially decaying components. The three decay times ranged from 6 to 8 ns, 1.8 to 3 ns, and 0.3 to 0.8 ns, depending on the emission wavelength. The fractional fluorescence of each component changed with incubation time. The long lifetime component had a reduced contribution to the total fluorescence while the short decay time component increased. The fluorescence spectra could be resolved into three distinct fluorescent components having maxima at 340 nm, 330 nm and 323 nm after 90 min of incubation, and 335 nm, 325 nm and 320 nm after 24 h of incubation. These maxima were, respectively, associated with the long, medium and short decay components. The fluorescence decay behaviour was interpreted as representing three families of tryptophans, the short lifetime component being due to a stacking interaction between tryptophan residues. The variation with incubation time suggests a two-step process in the channel-lipid organization. The first is associated with the conformational change of the polypeptide as it takes up a left-handed helical head-to-head dimer structure in the lipid. The second step is proposed to involve changes originating from membrane assembly and intermolecular interactions between channels as they form hexameric clusters.     

Detection of a pH-dependent conformational change in azurin by time-resolved phosphorescence.

Azurin, a blue copper protein from the bacterial species Pseudomonas aeruginosa, contains a single tryptophan residue. Previous fluorescence measurements indicate that this residue is highly constrained and unusually inaccessible to water. In the apoprotein this residue also possesses a long-lived room-temperature phosphorescence (RTP), the nonexponential decay of which can be resolved into two major components associated with lifetimes of 417 and 592 ms, which likely originate from at least two conformations of the protein. The relative weights of these two decay components change with pH in good correlation with a change in protonation of His-35, which has been studied in Cu(II) azurin. Interestingly, the structural changes characterized in earlier work have little effect on the fluorescence decay and appear to occur away from the tryptophan residue. However, in the present work, the two RTP lifetimes suggest conformations with different structural rigidities in the vicinity of the tryptophan residue. The active conformation that predominates below a pH of 5.6 has the shorter lifetime and is less rigid. Phosphorescence decays of several metal derivatives of azurin were also measured and revealed strong similarities to that of apoazurin, indicating that the structural constraints upon the metal-binding site are imposed predominately by the protein.     

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.     

Frequency domain measurements of the fluorescence lifetime of ribonuclease T1.

Using multifrequency phase/modulation fluorometry, we have studied the fluorescence decay of the single tryptophan residue of ribonuclease T1 (RNase T1). At neutral pH (7.4) we find that the decay is a double exponential (tau 1 = 3.74 ns, tau 2 = 1.06 ns, f1 = 0.945), in agreement with results from pulsed fluorometry. At pH 5.5 the decay is well described by a single decay time (tau = 3.8 ns). Alternatively, we have fitted the frequency domain data by a distribution of lifetimes. Temperature dependence studies were performed. If analyzed via a double exponential model, the activation energy for the inverse of the short lifetime component (at pH 7.4) is found to be 3.6 kcal/mol, as compared with a value of 1.0 kcal/mol for the activation energy of the inverse of the long lifetime component. If analyzed via the distribution model, the width of the distribution is found to increase at higher temperature. We have also repeated, using lifetime measurements, the temperature dependence of the acrylamide quenching of the fluorescence of RNase T1 at pH 5.5. We find an activation energy of 8 kcal/mol for acrylamide quenching, in agreement with our earlier report.     

Tryptophanyl fluorescence lifetime distribution of hyperthermophilic beta-glycosidase from molecular dynamics simulation: a comparison with the experimental data

A molecular dynamics simulation approach has been utilized to understand the unusual fluorescence emission decay observed for beta-glycosidase from the hyperthermophilic bacterium Solfolobus sulfotaricus (Sbeta gly), a tetrameric enzyme containing 17 tryptophanyl residues for each subunit. The tryptophanyl emission decay of Sbeta gly results from a bimodal distribution of fluorescence lifetimes with a short-lived component centered at 2.5 ns and a long-lived one at 7.4 ns (Bismuto E, Nucci R, Rossi M, Irace G, 1999, Proteins 27:71-79). From the examination of the trajectories of the side chains capable of causing intramolecular quenching for each tryptophan microenvironment and using a modified Stern-Volmer model for the emission quenching processes, we calculated the fluorescence lifetime for each tryptophanyl residue of Sbeta gly at two different temperatures, i.e., 300 and 365 K. The highest temperature was chosen because in this condition Sbeta gly evidences a maximum in its catalytic activity and is stable for a very long time. The calculated lifetime distributions overlap those experimentally determined. Moreover, the majority of trytptophanyl residues having longer lifetimes correspond to those originally identified by inspection of the crystallographic structure. The tryptophanyl lifetimes appear to be a complex function of several variables, such as microenvironment viscosity, solvent accessibility, the chemical structure of quencher side chains, and side-chain dynamics. The lifetime calculation by MD simulation can be used to validate a predicted structure by comparing the theoretical data with the experimental fluorescence decay results.     

Molecular mechanics analysis of Tet repressor TRP-43 fluorescence.

A 35% decrease in the fluorescence intensity of F75 TetR Trp-43 was observed upon binding of the tetracycline derivative 5a,6-anhydrotetracycline (AnTc) to the repressor. The fluorescence decay of Trp-43 in F75 TetR and in its complex with AnTc could be described by the sum of three exponential components, with lifetimes of about 6, 3, and 0.3 ns. The amplitudes, however, were markedly altered upon binding. The minimized energy mapping of Trp-43 chi 1 x chi 2 isomerization clearly indicated the existence of three main potential wells at positions (-160 degrees, -90 degrees) (rotamer I), (-170 degrees, 90 degrees) (rotamer II), and (-70, 150 degrees) (rotamer III). Our study of Trp-43 environment for each of the three rotamers suggests that the longest decay component may be assigned to rotamer II, the middle-lived component to rotamer I, and the subnanosecond component to rotamer III. The origin of the changes in the rotamer distribution upon AnTc binding is discussed. Anisotropy decays are also discussed within the framework of the rotamer model.     

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.