Anisotropy decays of single tryptophan proteins measured by GHz frequency-domain fluorometry with collisional quenching

We used harmonic-content frequency-domain fluorometry to determine the anisotropy decays of a variety of single tryptophan peptides and proteins. Resolution of the rapid and complex anisotropy decays was enhanced by global analysis of the data measured in the presence of quenching by either oxygen or acrylamide. For each protein, and for each quencher, data were obtained at four to six quencher concentrations, and the data analyzed globally to recover the anisotropy decay. The decrease in decay times produced by quenching allows measurements to an upper frequency limit of 2 GHz. The chosen proteins provided a range of exposures of the tryptophan residues to the aqueous phase, these being ACTH, monellin, Staphylococcus nuclease and ribonuclease T ₁, in order of decreasing exposure. Examination of indole and several small peptides demonstrates the resolution limitations of the measurements; a correlation time of 12 ps was measured for indole in methanol at 40°C. Comparison of the anisotropy decays of gly-trp-gly with leu-trp-leu revealed stearic effects of the larger leucine side chains on the indole ring. The anisotropy decay of gly-trp-gly revealed a 40 ps component for the indole side chain, which was resolved from the overall 150 ps correlation time of the tripeptide. Only the longer correlation time was observed for leu-trp-leu. With the exception of ribonuclease T ₁, each of the proteins displayed a subnanosecond component in the anisotropy decay which we assign to independent motions of the tryptophan residues. For example, Staphylococcus nuclease and monellin displayed segmental tryptophan motions with correlation times of 80 and 275 ps, respectively. The amplitudes of the rapid components increased with increasing exposure to the aqueous phase. These highly resolved anisotropy decays for proteins of known structure are suitable for comparison with molecular dynamic simulations.Abbreviations Ac acrylamide - ACTH adrenocorticotropin hormone (1–24) - BPTI bovine pancreatic trypsin inhibitor - NATA N-acetyl-L-tryptophanamide - RNase T ₁ ribonuclease T ₁ - S. Nuclease staphylococcus aureus nuclease Supported by grants DMB-8804931 and DIR-8710401 from the National Science Foundation, and GM-39617 from the National Institutes of Health. J. R. Lakowicz acknowledges support from the Medical Biotechnology Center at the University of Maryland. I. Gryczynski was on leave from University of Gáansk, Institute of Experimental Physics, Gdansk, Poland, with partial support from CPBP 01.06.2.01 (Poland). H. Cherek was on leave from Nicholas Copernicus University, Torun, Poland, with partial support from CPBP 01.06.2.03 Offprint requests to: J. R. Lakowicz     

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.     

Picosecond resolution of tyrosine fluorescence and anisotropy decays by 2-GHz frequency-domain fluorometry

We extended the technique of frequency-domain fluorometry to an upper frequency limit of 2000 MHz. This was accomplished by using the harmonic content of a laser pulse train (3.76 MHz, 5 ps) from a synchronously pumped and cavity-dumped dye laser. We used a microchannel plate photomultiplier as the detector to obtain the 2-GHz bandwidth. This new instrument was used to examine tyrosine intensity and anisotropy decays from peptides and proteins. These initial data sets demonstrate that triply exponential tyrosine intensity decays are easily recoverable, even if the mean decay time is less than 1 ns. Importantly, the extended frequency range provides good resolution of rapid and/or multiexponential tyrosine anisotropy decays. Correlation times as short as 15 ps have been recovered for indole, with an uncertainty of +/- 3 ps. We recovered a doubly exponential anisotropy decay of oxytoxin (29 and 454 ps), which probably reflects torsional motions of the phenol ring and overall rotational diffusion, respectively. Also, a 40-ps component was found in the anisotropy decay of bovine pancreatic trypsin inhibitor, which may be due to rapid torsional motions of the tyrosine residues and/or energy transfer among these residues. The rapid component has an amplitude of 0.05, which is about 16% of the total anisotropy. The availability of 2-GHz frequency-domain data extends the measurable time scale for fluorescence to overlap with that of molecular dynamics calculations.     

Measurement of subnanosecond anisotropy decays of protein fluorescence using frequency-domain fluorometry

We report the first anisotropy decays of protein fluorescence obtained using a frequency-domain fluorometer. The ultraviolet light source (300 nm) was a ring dye laser equipped with an intracavity frequency doubler, pumped by an argon ion laser. The data, measured at modulation frequencies from 2 to 200 MHz, reveal the presence of subnanosecond motions (0.1-0.2 ns) of the single tryptophan residues in melittin and monellin. For melittin the data also indicate the presence of slower motions near 1 ns, which may be the result of concerted motions of several peptide units. Smaller amplitude motions, on a similar timescale, were observed for the single tryptophan residue in staphylococcal nuclease. We demonstrate using N-acetyl-L-tryptophanamide in water that the method of frequency-domain fluorometry is capable of measuring correlation times as short as 50 ps. This method can provide data for the direct comparison of measured anisotropy decays with those predicted from molecular dynamics calculations.     

Intensity and anisotropy decays of the Wye base of yeast tRNA(Phe) as measured by frequency-domain fluorometry

The intensity and anisotropy decays of Wye base fluorescence from yeast tRNA(Phe) were determined by frequency-domain fluorometry. The intensity decay is at least a double exponential in the presence and absence of Mg2+, but the multi-exponential character of the decay is more pronounced in the absence of Mg2+. The anisotropy decay displays components due to overall tRNA rotational diffusion and to local torsional motions. The amplitude of the local motion is decreased 2-fold by the presence of Mg2+. The results are broadly consistent with a more homogeneous environment for the Wye base in the presence of Mg2+.     

A study of protein dynamics from anisotropy decays obtained by variable frequency phase-modulation fluorometry: internal motions of N-methylanthraniloyl melittin

Internal motions of melittin and its lipid complexes were studied by anisotropy decays determined by frequency-domain fluorometry. A covalent anthraniloyl probe was attached, probably to lysine-21. The emission spectra indicate that the anthraniloyl moiety is exposed to solvent in both monomeric and tetrameric forms and is present at the lipid-water interfacial region in the lipid complexes. The fluorescence intensity decay of melittin in solution and its lipid complexes was characterized by three lifetimes. The lifetimes were near 1-2 ns, 6-7 ns and 10 ns. At increased temperatures there was an increase in the amplitude of the intermediate lifetime and a decrease in that of the longer lifetime. For all the melittin systems, at least three correlation times were required to fit the anisotropy data. Of the three correlation times, the shortest correlation time represents the local motions of the probe, while the longest represents global motions of the whole molecule. The intermediate correlation time probably represents the dynamics of domains/helices within the molecule. The melittin monomer is highly flexible, with greater than 90% of its anisotropy being lost by the local motions. Even though it is well organized (greater than 75% helical), the tetramer is still a highly flexible molecule, with 70% of its anisotropy being lost by the local motions. The internal motions of melittin decrease upon binding to lipids and are sensitive to the phase state of the lipid complexes.     

Demonstration of an associated anisotropy decay by frequency-domain fluorometry

We used frequency-domain fluorometry to demonstrate the presence of an associated decay of fluorescence anisotropy. In such systems the individual correlation times are associated with distinct emitting species, each with its own characteristic lifetime and rotational correlation times. We obtained an associated system using 1-anilino-8-naphthalenesulfonic acid (ANS) in the presence of increasing amounts of apomyoglobin. When both free and apomyoglobin-bound ANS contributed to the emission the differential polarized phase angles become negative at particular frequencies, even though the fundamental anisotropy (r0) is greater than zero. Additionally, the modulated anisotropy decreases at high frequencies. Both observations appear to be the unique consequence of an associated anisotropy decay, and are not possible for a multiexponential anisotropy decay of a single species.     

Distribution of distances in thiopeptides by fluorescence energy transfer and frequency-domain fluorometry

Frequency-domain fluorescence spectroscopy was employed to examine the decays of tryptophan in Boc-Trp-Met-Asp-Phe-NH2 (donor) and (Formula: see text) (donor-acceptor pair). The efficiency of energy transfer in the thiopeptide amounted to 60%. The measured dispersion of fluorescence decay times was used to recover the donor-acceptor distance distribution. The parameters of the Gaussian distance distribution obtained for this peptide (r, the mean distance (9 A); hw, the halfwidth (25 A)) indicate the lack of a distinct favorable conformation.     

Picosecond resolution of oxytocin tyrosyl fluorescence by 2 GHz frequency-domain fluorometry

The technique of frequency-domain fluorometry has been extended to 2000 MHz using the harmonic content of a picosecond laser source and a microchannel plate photomultiplier tube. This new instrument was used to resolve complex subnanosecond intensity and anisotropy decays of the tyrosyl emission of oxytocin. The intensity decay was found to contain at least three exponential components, 80, 359 and 927 ps. The anisotropy analysis revealed a 29 ps torsional motion of the tyrosine residue as well as a 454 ps overall rotational correlation time. The time resolution of this method should permit the comparison of experimental results with theoretical models for motions of proteins.     

Anisotropy decay of diphenylhexatriene in melittin-phospholipid complexes by multifrequency phase-modulation fluorometry

Frequency-domain fluorometry was used to investigate the intensity and anisotropy decays of diphenylhexatriene (DPH) in melittin-lipid complexes. Simulated and experimental data indicate that correlation times ranging from 0.3 to 500 ns can be determined using data from 1 to 200 MHz. For the melittin-lipid complexes the hindered rotator model was not adequate to account for the anisotropy decays, especially at temperatures above the transition temperatures. At high protein-to-lipid ratios the data revealed the formation of small particles (100 A) of melittin and dipalmitoylphosphatidylcholine and the disruption of membrane order in bilayers of dipalmitoylphosphatidic acid.     

Influence of end-to-end diffusion on intramolecular energy transfer as observed by frequency-domain fluorometry

We investigated the influence of end-to-end diffusion on intramolecular energy transfer between a naphthalene donor and dansyl acceptor linked by polymethylene chain. A range of viscosities from 0.6 to 200 cP were obtained using propylene glycol at different temperatures (0-80 degrees C) and methanol at 20 degrees C. The intensity decays of naphthalene were measured in the frequency domain. Several theoretical models, including distance distributions, were used to fit the data. The results indicate that end-to-end diffusion of flexible donor-acceptor pairs can be detected and quantified using frequency-domain fluorometry, even in the presence of a distribution of donor-to-acceptor distances.     

Correction for incomplete labeling in the measurement of distance distributions by frequency-domain fluorometry.

Measurements of time-resolved fluorescence are now being used to recover conformational distributions of biological macromolecules. The fluorescence data of the donor are easily corrupted by incomplete labeling of the macromolecules by the acceptor. In the present paper we describe a general procedure to correct for incomplete acceptor labeling in the determination of distance distributions from frequency-domain measurements of the donor fluorescence decay kinetics. The method can also be used to determine the extent of acceptor labeling. Simulated data were used to determine the effect of incomplete labeling on resolution of the distance distribution and the effect on the recovered distributions if one fails to account for incomplete labeling by the acceptor. The expressions and implemented algorithm were verified using known mixtures of donor-control and donor-acceptor pair molecules, which simulated the presence of a donor population lacking the acceptor. Finally, we present data on the distance distributions between two labeled sites in myosin S1 (Cys-697 to Cys-707) where it was not possible to obtain complete labeling of the acceptor site.     

Intensity and anisotropy decays of the tyrosine calmodulin proteolytic fragments, as studied by GHz frequency-domain fluorescence

Frequency-domain fluorescence measurements to 2 GHz were able to recover and account for essentially all of the intrinsic tyrosine anisotropy of calmodulin and its proteolytic fragments containing one or two tyrosine residues. Low-temperature measurements have detected a very rapid initial anisotropy decay in the 2-tyrosine species which may be attributed to radiationless energy transfer between the two tyrosines. The observed values of the rotational correlation times indicate that both tyrosines of calmodulin possess considerable mobility, which decreases in the presence of Ca2+ and at low temperatures.     

Resolution of complex anisotropy decays by variable frequency phase-modulation fluorometry: a stimulation study

We used simulations to determine the resolution of complex anisotropy decay laws which is obtainable by frequency-domain fluorometry. The simulations include the effects of torsional and segmental motions of tryptophan residues in proteins, the multiple correlation times of asymmetric molecules, and three-component anisotropy decays. For a protein with a global correlation time of 10 ns it should be possible to resolve torsional motions with correlation times as short as 10 ps if the amplitude of the rapid motion is at least 20% of the total anisotropy decay with r0 = 0.4. Correlation times which differ by only 1.4-fold can be resolved, making this method useful for determination of the shape of proteins and other asymmetric molecules. It is possible to resolve three-component anisotropy decays if the overall difference among the correlation times is 30-fold. Such resolution will be useful for understanding of internal motions of proteins and membranes. The validity of these predictions is demonstrated in the subsequent paper using experimental data for melittin in solution and when bound to membranes (Maliwal, B.P., Hermetter, A. and Lakowicz, J.R. (1986) Biochim. Biophys. Acta 873, 173-181).     

Resolution of the conformational distribution and dynamics of a flexible molecule using frequency-domain fluorometry

We report the first resolution of both the conformational distribution and end-to-end diffusion coefficient of a flexible molecule. This molecular information was recovered using only the donor intensity decay in a single solvent at a single viscosity, as observed by the technique of frequency-domain fluorometry. This technique can be extended to measurements of structural fluctuations of biological macromolecules.     

Kinetic analysis of R67 dihydrofolate reductase folding: from the unfolded monomer to the native tetramer

R67 dihydrofolate reductase (DHFR) is a homotetrameric enzyme. Its subunit has a core structure consisting of five antiparallel beta-strands that form a compact beta-barrel. Our interest was to describe the molecular mechanism of the complete folding pathway of this beta-sheet protein, focusing on how the oligomerization steps are coordinated with the formation of secondary and tertiary structures all along the folding process. The folding kinetics of R67 dihydrofolate reductase into dimers at pH 5.0 were first examined by intrinsic tryptophan fluorescence, fluorescence energy transfer, and circular dichroism spectroscopy. The process was shown to consist of at least four steps, including a burst, a rapid, a medium, and a slow phase. Measurements of the ellipticity at 222 nm indicated that about 50% of the total change associated with refolding occurred during the 4 ms dead time of the stopped-flow instrument, indicating a substantial burst of secondary structure. The bimolecular association step was detected using fluorescence energy transfer and corresponded to the rapid phase. The slow phase was attributed to a rate-limiting isomerization of peptidyl-prolyl bonds involving 15% of the unfolded population. A complete folding pathway from the unfolded monomer to the native tetramer was proposed and an original model based upon the existence of early partially folded monomeric intermediates, rapidly stabilized in a dimeric form able to self-associate into the native homotetramer was formulated. The rate constants of these various steps were determined by fitting the kinetic traces to this model and supported our mechanistic assumptions.     

Anisotropy of the fluorescence from the monomer,five oligomers,and a polymer of epicatechin

The steady-state fluorescence anisotropy r has been measured at 25°C for dilute solutions of epicatechin units connected by interflavan bonds with 4β → 8 stereochemistry. The molecules studied are monodisperse oligomers from the monomer through the hexamer, and a polydisperse sample with a number-average degree of polymerization x_n of 10. The hexamer and smaller oligomers have been removed from the polydisperse sample. All samples have a very small value of r in 1,4-dioxane and in methanol. Higher values of r are seen in ethylene glycol and in glycerol. In the latter two solvents, the monomer has significantly higher r than any species with x_n > 1. This observation is interpreted as evidence for the presence of excitation migration from one monomer to another in the dimer and species of higher x_n.     

Human beta-tryptase: detection and characterization of the active monomer and prevention of tetramer reconstitution by protease inhibitors

beta-Tryptase is a trypsin-like serine protease stored in mast cell secretory granules primarily as an enzymatically active tetramer. The current study aims to determine whether monomeric beta-tryptase also can exhibit enzyme activity, as suggested previously. At neutral pH beta-tryptase tetramers in the absence of heparin or dextran sulfate spontaneously convert to inactive monomers. Addition of a polyanion to these monomers at neutral pH fails to convert them back to a tetramer or to an enzymatically active state. In contrast, at acidic pH addition of a polyanion resurrects enzyme activity. Whether this activity is associated with tetramers or monomers depends on the concentration of beta-tryptase. Under the experimental conditions employed at pH 6 in the presence of heparin, the monomer concentration at which 50% conversion to tetramers occurs is 193 ng/mL. Activity against tripeptide substrates by monomers is detected at pH 6 but not at pH 7.4, whereas tetramer activity is greater at pH 7.4 than pH 6.0. Active monomers are inhibited by soybean trypsin inhibitor, bovine pancreatic trypsin inhibitor, antithrombin III, and alpha2-macroglobulin, whereas active tetramers are resistant to these inhibitors. Active monomers form complexes with these inhibitors and cleave both antithrombin III and alpha2-macroglobulin. These inhibitors also prevent reconstitution of monomers to tetramers, indicating that inactive monomers become active monomers before becoming active tetramers. The ability of tryptase monomers to become active at acidic pH raises the possibilities of expanded substrate specificities as well as inhibitor susceptibilities where the low-pH environments associated with inflammation or poor vascularity are encountered in vivo.