Picosecond time-resolved fluorescence of ribonuclease T1. A pH and substrate analogue binding study.

The tryptophyl fluorescence of ribonuclease T1 decays monoexponentially at pH 5.5, tau = 4.04 ns but on increasing pH, a second short-lived component of 1.5 ns appears with a midpoint between pH 6.5 and 7.0. Both components have the same fluorescence spectrum. Acrylamide quenches both fluorescence components, and the short-lived component is quenched fivefold faster than the predominant long component. Binding of the substrate analogue 2'-guanylic acid at pH 5.5 quenches the fluorescence by 20% and introduces a second decay component, tau = 1.16 ns. Acrylamide quenches both tryptophyl decay components, with similar quenching rates. The fluorescence anisotropy decay of ribonuclease T1 was consistent with a molecule the size of ribonuclease T1 surrounded by a single layer of water at pH 7.4, even though the anisotropy decay at pH 5.5 deviated from Stokes-Einstein behavior. The fluorescence data were interpreted with a model where the tryptophyl residue exists in two conformations, remaining in a hydrophobic pocket. The acrylamide quenching is interpreted with electron transfer theory and suggests that one conformer has the nearest atom approximately 3 A from the protein surface, and the other, approximately 2 A.     

Acrylamide and oxygen fluorescence quenching studies with liver alcohol dehydrogenase using steady-state and phase fluorometry

The fluorescence lifetime of liver alcohol dehydrogenase (LADH) has been determined by phase fluorometry at various emission wavelengths and as a function of the concentration of the quencher acrylamide. Acrylamide selectively quenches the fluorescence of the surface tryptophanyl residue Trp-15, thus allowing the fluorescence lifetime of this residue and the buried residue Trp-314 to be evaluated. Values of tau15 = 6.9 ns and tau314 = 3.6 ns are obtained, in qualitative agreement with lifetimes of these residues determined from fluorescence decay studies [Ross, J.B.A., Schmidt, C.J., & Brand, L. (1981) Biochemistry 20, 4369-4377]. The quenching of the fluorescence of LADH by oxygen has also been studied. Quenching by oxygen results in a blue shift in the fluorescence of the protein and a downward-curving Stern-Volmer plot. These data, along with oxygen quenching studies in the presence of 1 M acrylamide, are consistent with a model in which oxygen quenches the fluorescence of Trp-314 and -15 with quenching constants of 3.5 and 25 M-1, respectively. Thus, as in studies with other quenchers, Trp-314 is found to be less accessible to the quencher oxygen than is Trp-15. A lifetime Stern-Volmer plot has also been obtained for the oxygen quenching of LADH. Such a plot deviates somewhat from the intensity Stern-Volmer plot as predicted by simulations of the quenching of two-component systems.     

Effect of micelle diameter on tryptophan dynamics in an amphipathic helical peptide in phosphatidylcholine

The effect of dimyristoylphosphatidylcholine (DMPC) on the conformation and environment of the single tryptophan residue of a model amphipathic helical polypeptide has been investigated by fluorescence quenching with a water-soluble, neutral quencher (acrylamide) and multiple-frequency phase fluorometry. The peptide H-Ser-Ser-Ala-Asp-Trp-Leu-Lys-Ala-Phe-Tyr-Asp-Lys-Val-Ala-Glu-Lys-Leu-Ly s-Glu- Ala-Phe-Ser-Ser-Ser-OH [18As; Kanellis, P., Romans, A.Y., Johnson, B.J., Kercret, H., Chiovetti, R., Jr., Allen, T.M., & Segrest, S.P. (1980) J. Biol. Chem. 255, 11464] was synthesized by solid-phase techniques. Peptide was incubated at 26 degrees C with DMPC at various peptide:lipid weight ratios. The diameter of the resulting disk-shaped micelles increases with increasing lipid concentration from 12.0 +/- 0.4 nm at a 1:1 weight ratio of peptide to lipid to a maximum of 48.7 +/- 1.0 nm at a 1:13 ratio. At a weight ratio of 1:5, the average diameter is 22.7 +/- 0.6 nm. Decreasing the peptide:lipid ratio of the micelle resulted in a blue-shift in the fluorescence emission maximum (from 337 nm at 1:1 to 334 nm at 1:5), an increase in the fluorescence lifetime of the tryptophan measured by the phase shift method at 18 MHz (from 3.12 ns at 1:1 to 3.61 ns at 1:5), a decrease in the rate of fluorescence quenching by acrylamide (from 0.87 x 10(9) M-1 s-1 at 1:1 to 0.42 x 10(9) M-1 s-1 at 1:5), and an increase in the activation energy for quenching (from 6.7 kcal/mol at 1:1 to 12.7 kcal/mol at 1:5).(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformational dynamics of bovine Cu, Zn superoxide dismutase revealed by time-resolved fluorescence spectroscopy of the single tyrosine residue.

The structural dynamics of bovine erythrocyte Cu, Zn superoxide dismutase (BSOD) was studied by time-resolved fluorescence spectroscopy. BSOD is a homodimer containing a single tyrosine residue (and no tryptophan) per subunit. Frequency-domain fluorometry revealed a heterogeneous fluorescence decay that could be described with a Lorentzian distribution of lifetimes. The lifetime distribution parameters (center and width) were markedly dependent on temperature. The distribution center (average lifetime) displayed Arrhenius behavior with an Ea of 4.2 kcal/mol, in contrast with an Ea of 7.4 kcal/mol for the single-exponential decay of L-tyrosine. This indicated that thermal quenching of tyrosine emission was not solely responsible for the effect of temperature on the lifetimes of BSOD. The distribution width was broad (1 ns at 8 degrees C) and decreased significantly at higher temperatures. Furthermore, the width of the lifetime distribution increased in parallel to increasing viscosity of the medium. The combined effects of temperature and viscosity on the fluorescence decay suggest the existence of multiple conformational substrates in BSOD that interconvert during the excited-state lifetime. Denaturation of BSOD by guanidine hydrochloride produced an increase in the lifetime distribution width, indicating a larger number of conformations probed by the tyrosine residue in the denatured state. The rotational mobility of the tyrosine in BSOD was also investigated. Analysis of fluorescence anisotropy decay data enabled resolution of two rotational correlation times. One correlation time corresponded to a fast (picosecond) rotation that contributed 62% of the anisotropy decay and likely reported local mobility of the tyrosine ring. The longer correlation time was 50% of the expected value for rotation of the whole (dimeric) BSOD molecule and appeared to reflect segmental motions in the protein in addition to overall tumbling. Comparison between rotational correlation times and fluorescence lifetimes of BSOD indicates that the heterogeneity in lifetimes does not arise from mobility of the tyrosine per se, but rather from dynamics of the protein matrix surrounding this residue which affect its fluorescence decay.     

Time-resolved fluorescence studies of dityrosine in the outer layer of intact yeast ascospores.

The (time-resolved) fluorescence properties of dityrosine in the outermost layer of the spore wall of Saccharomyces cerevisiae were investigated. Steady-state spectra revealed an emission maximum at 404 nm and a corresponding excitation maximum at 326 nm. The relative fluorescence quantum yield decreased with increasing proton concentration. The fluorescence decay of yeast spores was found to be nonexponential and differed pronouncedly from that of unbound dityrosine in water. Analysis of the spore decay recorded at lambda ex = 323 nm and lambda em = 404 nm by an exponential series (ESM) algorithm revealed a bimodal lifetime distribution with maxima centered at tau 1C = 0.5 ns and tau 2C = 2.6 ns. The relative amplitudes of the two distributions are shown to depend on the emission wavelength, indicating contributions from spectrally different dityrosine chromophores. On quenching the spore fluorescence with acrylamide, a downward curvature of the Stern-Volmer plot was obtained. A multitude of chromophores more or less shielded from solvent in the spore wall is proposed to account for the nonlinear quenching of the total spore fluorescence. Analysis of the fluorescence anisotropy decay revealed two rotational correlation times (phi 1 = 0.9 ns and phi 2 = 30.6 ns) or a bimodal distribution of rotational correlation times (centers at 0.7 ns and 40 ns) when the data were analyzed by the maximum entropy method (MEM). We present a model that accounts for the differences between unbound (aqueous) and bound (incorporated in the spore wall) dityrosine fluorescence. The main feature of the photophysical model for yeast spores is the presence of at least two species of dityrosine chromophores differing in their chemical environments. A hypothetical photobiological role of these fluorophores in the spore wall is discussed: the protection of the spore genome from mutagenic UV light.     

Contribution of histidine residues to the conformational stability of ribonuclease T1 and mutant Glu-58----Ala

The pK values of the histidine residues in ribonuclease T1 (RNase T1) are unusually high: 7.8 (His-92), 7.9 (His-40), and 7.3 (His-27) [Inagaki et al. (1981) J. Biochem. 89, 1185-1195]. In the RNase T1 mutant Glu-58----Ala, the first two pK values are reduced to 7.4 (His-92) and 7.1 (His-40). These lower pKs were expected since His-92 (5.5 A) and His-40 (3.7 A) are in close proximity to Glu-58 at the active site. The conformational stability of RNase T1 increases by over 4 kcal/mol between pH 9 and 5, and this can be entirely accounted for by the greater affinity for protons by the His residues in the folded protein (average pK = 7.6) than in the unfolded protein (pk approximately 6.6). Thus, almost half of the net conformational stability of RNase T1 results from a difference between the pK values of the histidine residues in the folded and unfolded conformations. In the Glu-58----Ala mutant, the increase in stability between pH 9 and 5 is halved (approximately 2 kcal/mol), as expected on the basis of the lower pK values for the His residues in the folded protein (average pK = 7.1). As a consequence, RNase T1 is more stable than the mutant below pH 7.5, and less stable above pH 7.5. These results emphasize the importance of measuring the conformational stability as a function of pH when comparing proteins differing in structure.     

Tracking local conformational changes of ribonuclease A using picosecond time-resolved fluorescence of the six tyrosine residues

The six tyrosine residues of ribonuclease A (RNase A) are used as individual intrinsic probes for tracking local conformational changes during unfolding. The fluorescence decays of RNase A are well described by sums of three exponentials with decay times (tau(1) = 1.7 ns, tau(2) = 180 ps, and tau(3) = 30 ps) and preexponential coefficients (A(1) = 1, A(2) = 1, and A(3) = 4) at pH 7, 25 degrees C. The decay times are controlled by photo-induced electron transfer from individual tyrosine residues to the nearest disulphide (-SS-), bridge, which is distance (R) dependent. We assign tau(1) to Tyr-76 (R = 12.8 A), tau(2) to Tyr-115 (R = 6.9 A), and tau(3) to Tyr-25, Tyr-73, Tyr-92, and Tyr-97 (all four at R = 5.5 +/- 0.3 A) at 23 degrees C. On the basis of this assignment, the results show that, upon thermal or chemical unfolding only Tyr-25, Tyr-92, and Tyr-76 undergo significant displacement from their nearest -SS- bridge. Despite reporting on different regions of the protein, the concordance between the transition temperatures, T(m), obtained from Tyr-76 (T(m) = 59.2 degrees C) and Tyr-25 and Tyr-92 (T(m) = 58.2 degrees C) suggests a single unfolding event in this temperature range that affects all these regions similarly.     

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.     

Fluorescence quenching of Trp-314 of liver alcohol dehydrogenase by oxygen

The quenching of the fluorescence of liver alcohol dehydrogenase (LADH) by molecular oxygen has been studied by both fluorescence lifetime and intensity measurements. This was done in the presence of 1 M acrylamide which selectively quenches the fluorescence of the surface tryptophan residue, Trp-15, thus allowing us to focus on the quenching of the deeply buried tryptophan, Trp-314, by molecular oxygen. Such studies yielded a Stern-Volmer plot of F0/F with a greater slope than the corresponding tau o/tau plot. This indicates that both dynamic and static quenching of Trp-314 occurs. The temperature dependence of the dynamic quenching of LADH by oxygen was also studied at three temperatures, from which we determined the activation enthalpy for the quenching of Trp-314 to be about 10 kcal/mol. The oxygen quenching of a ternary complex of LADH, NAD+ and trifluoroethanol was also studied. The rate constant for dynamic quenching of Trp-314 by oxygen was found to be approximately the same in the ternary complex as that in the unliganded enzyme.     

Conformational stability and mechanism of folding of ribonuclease T1

Urea and thermal unfolding curves for ribonuclease T1 (RNase T1) were determined by measuring several different physical properties. In all cases, steep, single-step unfolding curves were observed. When these results were analyzed by assuming a two-state folding mechanism, the plots of fraction unfolded protein versus denaturant were coincident. The dependence of the free energy of unfolding, delta G (in kcal/mol), on urea concentration is given by delta G = 5.6 - 1.21 (urea). The parameters characterizing the thermodynamics of unfolding are: midpoint of the thermal unfolding curve, Tm = 48.1 degrees C, enthalpy change at Tm, delta Hm = 97 kcal/mol, and heat capacity change, delta Cp = 1650 cal/mol deg. A single kinetic phase was observed for both the folding and unfolding of RNase T1 in the transition and post-transition regions. However, two slow kinetic phases were observed during folding in the pre-transition region. These two slow phases account for about 90% of the observed amplitude, indicating that a faster kinetic phase is also present. The slow phases probably result from cis-trans isomerization at the 2 proline residues that have a cis configuration in folded RNase T1. These results suggest that RNase T1 folds by a highly cooperative mechanism with no structural intermediates once the proline residues have assumed their correct isomeric configuration. At 25 degrees C, the folded conformation is more stable than the unfolded conformations by 5.6 kcal/mol at pH 7 and by 8.9 kcal/mol at pH 5, which is the pH of maximum stability. At pH 7, the thermodynamic data indicate that the maximum conformational stability of 8.3 kcal/mol will occur at -6 degrees C.     

Time-resolved fluorescence of DAPI in solution and bound to polydeoxynucleotides

Fluorescence decay studies, obtained by multifrequency phase-modulation fluorometry, have been performed on DAPI in solution and complexed with natural and synthetic polydeoxynucleotides. DAPI decay at pH 7 was decomposed using two exponential components of 2.8 and 0.2 ns of lifetime values, respectively. The double exponential character of the decay was maintained over a large pH range. Phase- and modulation-resolved spectra, collected between 420 and 550 nm, have indicated at least two spectral components associated with the two lifetime values. This, plus the observation of the dependence of the emission spectrum on the excitation wavelength, suggests a lifetime heterogeneity originating from ground-state molecular conformers, partially affected by pH changes. DAPI complexed with natural polydeoxynucleotides retained most of the features of DAPI decay in solution, except for the value of the long lifetime component that was longer (approximately 4 ns) and the relative fractional fluorescence intensities of the two components that were inverted. AT polymers/DAPI complexes show single exponential decay. Solvent shielding when DAPI is bound to DNA changes the indole ring solvation and stabilizes the longer lifetime decay component. For poly(GC)/DAPI complex, the decay was similar to that of free DAPI in solution, proving the dependence on the polydeoxynucleotides sequence the different types of binding and the reliability of the fluorescence method to solve them.     

Fluorescence lifetime distributions of diphenylhexatriene-labeled phosphatidylcholine as a tool for the study of phospholipid-cholesterol interactions.

Fluorescence lifetimes of 1-palmitoyl-2-diphenylhexatrienylpro-pionyl-phosphatidylc hol ine in vesicles of palmitoyloleoyl phosphatidylcholine (POPC) (1:300, mol/mol) in the liquid crystalline state were determined by multifrequency phase fluorometry. On the basis of statistic criteria (chi 2red) the measured phase angles and demodulation factors were equally well fitted to unimodal Lorentzian, Gaussian, or uniform lifetime distributions. No improvement in chi 2red could be observed if the experimental data were fitted to bimodal Lorentzian distributions or a double exponential decay. The unimodal Lorentzian lifetime distribution was characterized by a lifetime center of 6.87 ns and a full width at half maximum of 0.57 ns. Increasing amounts of cholesterol in the phospholipid vesicles (0-50 mol% relative to POPC) led to a slight increase of the lifetime center (7.58 ns at 50 mol% sterol) and reduced significantly the distributional width (0.14 ns at 50 mol% sterol). Lifetime distributions of POPC-cholesterol mixtures containing greater than 20 mol% sterol were within the resolution limit and could not be distinguished from monoexponential decays on the basis of chi 2red. Cholesterol stabilizes and rigidifies phospholipid bilayers in the fluid state. Considering its effect on lifetime distributions of fluorescent phospholipids it may also act as a membrane homogenizer.     

Lifetime and quenching of tryptophan fluorescence in whiting parvalbumin

The fluorescence lifetime of the single tryptophan in whiting parvalbumin has been measured by time-correlated single-photon counting. In the presence of saturating calcium, greater than 2 mol/mol of protein, the decay of fluorescence is accurately single exponential with a lifetime of 4.6 ns (0.1 M KCl, 20 mM borate, 1 mM dithiothreitol, 20 degrees C, pH 9). Upon complete removal of calcium from parvalbumin with ethylene glycol bis(beta-aminoethyl ether)-N,N,N',N'-tetraacetic acid the emission decay becomes biphasic, and a second more rapid decay process with a lifetime of 1.3 ns comprising approximately 18% of the fluorescence emission at 350 nm is observed. The fluorescence emission of the calcium-saturated form is not measurably quenched by iodide. In contrast, upon complete removal of calcium, the fluorescence is completely quenchable as shown by extrapolation of the data to infinite iodide concentration. These results indicate that there is a large increase in the accessibility of the tryptophan residue in the protein to solvent upon removal of calcium. Stern-Volmer plots of the quenching data are nonlinear and indicate that there is more than one quenchable conformation of the calcium-free protein. The lifetime and quenching results are consistent with the presence of significant concentrations of only two stoichiometric species, apoparvalbumin and parvalbumin--Ca2, at partial occupancy of the calcium binding sites.     

Fluorescence studies of the conformational dynamics of parvalbumin in solution: lifetime and rotational motions of the single tryptophan residue

The fluorescence properties of the single tryptophan residue in whiting parvalbumin were used to probe the dynamics of the protein matrix. Ca2+ binding caused a blue-shift in the emission (from lambda max = 339 to 315 nm) and a 2.5-fold increase in quantum yield. The fluorescence decay was nonexponential in both Ca2(+)-free and Ca2(+)-bound parvalbumin and was best described by Lorentzian lifetime distributions centered around two components: a major long-lived component at 2-5 ns and a small subnanosecond component. Raising the temperature from 8 to 45 degrees C resulted in a decrease in both the center (average) and width (dispersion) of the major lifetime distribution component, whereas the center, width, and fractional intensity of the fast component increased with temperature. Arrhenius activation energies of 1.3 and 0.3 kcal/mol were obtained in the absence and in the presence of Ca2+, respectively, from the temperature dependence of the center of the major lifetime distribution component. Direct anisotropy decay measurements of local tryptophan rotations yielded an activation energy of 2.3 kcal/mol in Ca2(+)-depleted parvalbumin and indicated a correlation between rotational rates and lifetime distribution parameters (center and width). Ca2+ binding produced a decrease in the width of the major lifetime distribution component and a decrease in tryptophan rotational mobility within the protein. There was a rough correlation between these two parameters with changes in Ca2+ and temperature, so that both measurements may be taken to indicate that the structure of Ca2(+)-bound parvalbumin was more rigid than in Ca2(+)-depleted parvalbumin.     

Lifetime distributions and anisotropy decays of indole fluorescence in cyclohexane/ethanol mixtures by frequency-domain fluorometry

We used frequency-domain fluorometry to measure intensity and anisotropy decay of indole fluorescence in cyclohexane/ethanol mixtures at 20 degrees C. In 100% cyclohexane or 100% ethanol the intensity decay of indole appears to be a single exponential with decay times of 7.66 and 4.10 ns, respectively. In cyclohexane containing a small percentage of ethanol (up to 10%), we observed increased heterogeneity in intensity decay, resulting in a 10-fold increase in chi 2R for the single-exponential fit, as compared with the double-exponential model. We obtained comparable or better fits using unimodal Lorentzian and Gaussian lifetime distributions (two floating parameters) than for the two-exponential model (three floating parameters). We believe that the distribution of decay times reflects a range of indole solvation states in the dominately nonpolar solutions. This result suggests that a variety of hydrogen-bonding configurations could be one origin of the distributions of decay times observed for tryptophan emission from proteins. We also measured rotational diffusion of indole in cyclohexane, ethanol and its mixtures at 20 degrees C. The picosecond correlation times required that the mean decay times be decreased by acrylamide quenching (in ethanol) or energy transfer (in cyclohexane). In ethanol we observed nearly isotropic rotation of indole; in cyclohexane we obtained two correlation times of 17 and 73 ps. The shorter correlation time in cyclohexane appears to be due to the slip boundary condition, which was found to be progressively eliminated by small percentages of ethanol. Hence, hydrogen-bonding interactions appear to have a substantial effect on the rotational dynamics of indole.     

Oxygen and acrylamide quenching of protein phosphorescence: correlation with protein dynamics

Oxygen quenching of protein phosphorescence and activation enthalpies for the structural fluctuations underlying O2 and acrylamide diffusion were determined for RNase T1, glyceraldehyde-3-phosphate dehydrogenase and beta-lactoglobulin, which have the phosphorescing residues located in relatively solvent-exposed and flexible regions of the polypeptide. The results, compared with those obtained for proteins characterised by a very rigid environment, established that kqO2 was directly correlated to the flexibility of the protein matrix surrounding the chromophore. While the migration of acrylamide was characterised by delta H(double dagger), which was strongly dependent on the fluidity of the structure about the Trp residue, the values of the activation enthalpies for the oxygen migration of all the proteins studied were rather similar, approximately 10 kcal mol(-1), in spite of the depth of the chromophore and the rigidity of its environment. The implications of these findings for the migration of small solutes inside proteins have been discussed.     

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.     

On the structure and conformational dynamics of yeast phenylalanine-accepting transfer ribonucleic acid in solution.

The solution structure of yeast tRNAPhe was investigated by using ethidium as a fluorescent probe in the D loop and the anticodon loop. For this purpose the dihydrouracils in position 16/17 and wybutine in position 37 were substituted by ethidium. The lifetimes and the time-dependent anisotropy of ethidium fluorescence were measured by pulsed nanosecond fluorometry. The kinetics of the transitions between different states of the tRNAPheEtd derivatives were determined by chemical relaxation measurements. It was found that the ethidium label irrespective of its position exhibits three different states called T1, T2 and T3 characterized by lifetimes tau 1 = 30 ns, tau 2 = 12 ns, and tau 3 = 3 ns. The lifetime differences are due to different accessibilities of ethidium for solvent quenching in the three states. Thus, there are three different defined structural environments of the ethidium in both the anticodon and the D loop. The distribution of the three states was measured as a function of Mg2+ concentration and temperature; it was found that state T3 is favored over states T2 and T1 by both increasing Mg2+ concentration and increasing temperature. The chemical relaxation kinetics exhibit a fast transition between T1 and T2 (10--100 ms) and a slow transition between T2 and T3 (100--1000 ms). The rates of both transitions depend likewise on Mg2+ concentration and temperature. The equilibrium and kinetic data clearly show the presence of strong and weak interactions between Mg2+ and tRNA. A cooperative model accounting for this behavior is developed. The ethidium probe behaves identically when located in different regions of the tRNA regarding both its distribution of states and its transition kinetics. This suggests that the different spectroscopic states report different conformations of the tRNA structure. The dependence of the three states on Mg2+ and spermine indicates that conformation T3 is closely related to or identical with the crystal structure. The rotational diffusion constants indicate that of all three states T3 is most extended while T2 is most compact. The thermodynamic analysis reveals that the strongly bound Mg2+ ions reduce both the activation entropy and enthalpy of all transitions. The weakly bound Mg2+ ions increase both the activation enthalpy and entropy of the slow transition between T2 and T3. It is suggested that the breaking of several intramolecular bonds, e.g., hydrogen bonds, is involved in this transition.     

The effect of cytochrome P-450cam on the NMR relaxation rate of water protons.

Cytochrome P-450cam in the native, substrate-free state (Fe3+, S = 1/2) substantially reduces the NMR relaxation times, T1 and T2, of water protons. Temperature and frequency dependences of T1 and T2 were measured; they are consistent with a model of one or two protons exchanging between a binding site on a heme ligand and bulk water. The relevant parameters of this model have been deduced from the data. The spin relaxation time of the heme iron, tau S similar to 0.5 ns at 25 degrees C, is unusually long for a low spin ferric heme protein but is compatible with the line widths measured for paramagnetically shifted heme resonances. The proton residence time on the ligand, tau M similar to 1 microsecond at 25 degrees C, follows an Arrhenius law with activation energy EM similar to 15 kcal/mol. A scalar hyperfine interaction A/h = 2.2 MHz (3.1 MHz for one-proton exchange) of the found proton(s) with the heme iron is deduced from the difference between T1 and T2 observed in the fast exchange limit. The iron-proton distance is found to be 2.9 A (2.6 A for one-proton exchange). Variation of pH between pH 6.4 and 8.6 does not affect T1. The bearing of these results on the question of the axial heme ligand is discussed.