Conformations of the core nucleosome: effects of ionic strength and high mobility group protein 14 and 17 binding on the fluorescence emission and polarization of dansylated methionine-84 of histone H4

Chicken histone H4 labeled at Met-84 with the fluor N-[(acetylamino)ethyl]-8-naphthyl-amine-1-sulfonic acid has been incorporated into a nucleosome which has physical characteristics virtually identical with those of native core nucleosomes. The fluorescence emission and polarization properties of the labeled nucleosome were measured as a function of ionic strength and the binding of high mobility group (HMG) proteins 14 and 17. Also, the accessibility of the fluor to the quenching agent acrylamide was determined. It was found that the fluorescence emission changes in the range 0.1-1000 mM NaCl are rather small and indicate that no major unfolding of the octamer structure occurs around Met-84 on H4 at least. Five or perhaps six discrete states were found in that ionic strength range. Each has a different accessibility to the quenching agent. The range of accessibilities varied from 9 X 10(-7) to 32 X 10(-7) mol-1 s-1 for 0.1-1000 mM NaCl, respectively. Polarization measurements showed that there was little change in the rotational relaxation lifetime of the fluor at ionic strengths less than 50 mM NaCl. Above this value, the rotational relaxation lifetimes decreased from 107 to 25 ns at 600 mM NaCl, indicating a moderately increased rotational freedom for the fluor. It is suggested that the histone octamer changes its degree of compaction in the range 0.1-600 mM NaCl but that no major protein unfolding occurs.(ABSTRACT TRUNCATED AT 250 WORDS)     

Rotational freedom of tryptophan residues in proteins and peptides

We studied the rotational motions of tryptophan residues in proteins and peptides by measurement of steady-state fluorescence anisotropies under conditions of oxygen quenching. By fluorescence quenching we can shorten the fluorescence lifetime and thereby decrease the average time for rotational diffusion prior to fluorescence emission. This method allowed measurement of rotational correlation times ranging from 0.03 to 50 ns, when the unquenched fuorescence lifetimes are near 4 ns. A wide range of proteins and peptides were investigated with molecular weights ranging from 200 to 80 000. Many of the chosen substances possessed a single tryptophan residue to minimize the uncertainties arising from a heterogeneous population of fluorophores. In addition, we also studied a number of multi-tryptophan proteins. Proteins were studied at various temperatures, under conditions of self-association, and in the presence of denaturants. A wide variety of rotational correlation times were found. As examples we note that the single tryptophan residue of myelin basic protein was highly mobile relative to overall protein rotation whereas tryptophan residues in human serum albumin, RNase T1, aldolase, and horse liver alcohol dehydrogenase were found to be immobile relative to the protein matrix. These results indicate that one cannot generalize about the extent of segmental mobility of the tryptophan residues in proteins. This physical property of proteins is highly variable between proteins and probably between different regions of the same protein.     

Fluorescence anisotropy decay of ethidium bound to nucleosome core particles. 1. Rotational diffusion indicates an extended structure at low ionic strength

The fluorescence decay of ethidium intercalated into the DNA of nucleosome core particles increases in average lifetime from about 22 ns in H2O to about 39 ns in D2O. This increase, combined with the acquisition of large amounts of data (on the order of 10(8) counts per decay), allows measurement of anisotropy decays out to more than 350 ns. The overall slow rotational motions of the core particle may thereby be more clearly distinguished from the faster torsional motions of the DNA. In 10 mM NaCl at 20 degrees C, we recover a long correlation time of 198 ns in D2O (159 ns when corrected to a viscosity of 1.002 cP), in agreement with the value of 164 ns obtained in H2O. These values are consistent with hydrodynamic calculations based on the expected size and shape of the hydrated particle. To support our conclusion that this long correlation time derives from Brownian rotational diffusion, we show that the value is directly proportional to the viscosity and inversely proportional to the temperature. No significant changes in the rotational correlation time are observed between 1 and 500 mM ionic strength. Below 1 mM, the particle undergoes the "low-salt transition" as measured by steady-state tyrosine fluorescence anisotropy. However, we observe little change in shape until the ionic strength is decreased below approximately 0.2 mM, where the correlation time increases nearly 2-fold, indicating that the particle has opened up into an extended form. We have previously shown that the transition becomes nonreversible below 0.2 mM salt.     

Analysis of hydride transfer and cofactor fluorescence decay in mutants of dihydrofolate reductase: possible evidence for participation of enzyme molecular motions in catalysis.

A remarkable correlation has been discovered between fluorescence lifetimes of bound NADPH and rates of hydride transfer among mutants of dihydrofolate reductase (DHFR) from Escherichia coli. Rates of hydride transfer from NADPH to dihydrofolate change by a factor of 1,000 for the series of mutant enzymes. Since binding constants for the initial complex between coenzyme and DHFR change by only a factor of 10, the major portion of the change in hydride transfer must be attributed to losses in transition-state stabilization. The time course of fluorescence decay for NADPH bound to DHFR is biphasic. Lifetimes ranging from 0.3 to 0.5 ns are attributed to a solvent-exposed dihydronicotinamide conformation of bound coenzyme which is presumably not active in catalysis, while decay times (tau 2) in the range of 1.3 to 2.3 ns are assigned to a more tightly bound species of NADPH in which dihydronicotinamide is sequestered from solvent. It is this slower component that is of interest. Ternary complexes with three different inhibitors, methotrexate, 5-deazafolate, and trimethoprim, were investigated, along with the holoenzyme complex; 3-acetylNADPH was also investigated. Fluorescence polarization decay, excitation polarization spectra, the temperature variation of fluorescence lifetimes, fluorescence amplitudes, and wavelength of absorbance maxima were measured. We suggest that dynamic quenching or internal conversion promotes decay of the excited state in NADPH-DHFR. When rates of hydride transfer are plotted against the fluorescence lifetime (tau 2) of tightly bound NADPH, an unusual correlation is observed. The fluorescence lifetime becomes longer as the rate of catalysis decreases for most mutants studied. However, the fluorescence lifetime is unchanged for those mutations that principally alter the binding of dihydrofolate while leaving most dihydronicotinamide interactions relatively undisturbed. The data are interpreted in terms of possible dynamic motions of a flexible loop region in DHFR which closes over both substrate and coenzyme binding sites. These motions could lead to faster rates of fluorescence decay in holoenzyme complexes and, when correlated over time, may be involved in other motions which give rise to enhanced rates of catalysis in DHFR.     

Structure and dynamics of motilin. Time-resolved fluorescence of peptide hormone with single tyrosine residue.

Time-resolved fluorescence and CD spectroscopy were used to characterize the structure and dynamics of the peptide hormone motilin with a single tyrosine residue among its 22 amino acids. CD spectroscopy showed that secondary structure is independent of concentration in the range 1 x 10(-5)-2.6 x 10(-4) M, and of the presence of DOPC lipid vesicles, but is strongly induced by addition of hexafluoroisopropanol. The fluorescence studies with tyrosine as the intrinsic fluorophore, performed at the MAX synchrotron laboratory at Lund, showed that three fluorescence lifetimes (0.4 ns, 1.7 ns and 3.6 ns at 20 degrees C) and two rotational correlation times (0.4 ns and 5 ns at 20 degrees C) were needed to account for the data. The different decay times are interpreted as representing ground-state rotamers interconverting slowly on the ns time scale. The rotational correlation times are ascribed to local angular motion of the tyrosyl ring, and global motion of the whole peptide, respectively.     

Dynamics of benzo[a]pyrene diol epoxide adducts in poly(dG-dC).(dG-dC) studied by synchrotron excited fluorescence polarization anisotropy decay.

Time-resolved fluorescence studies have been performed on (+)-anti-7,8-dihydrodiol-9,10-epoxybenzo[a]pyrene adducts in double-stranded poly(dG-dC).(dG-dC). Part of the adduct population gives rise to excimer fluorescence. The heterogeneous fluorescence emission decay curves at 22 degrees C could be resolved into three components with lifetimes: 0.4 ns, 3 ns and 24 ns for the total fluorescence (monomer and excimer emission), and 0.5 ns, 5 ns and 24 ns, respectively, for excimer emission alone. The relative amplitudes for the longer lifetimes were larger for the pure excimer population than for the mixed population. The fluorescence polarization anisotropy decay curves were resolved into two components of rotational correlation times: 0.4 ns and 25 ns for the total fluorescence and 0.3 ns and 33 ns for the excimer fluorescence. We interpret the two rotational correlation times to correspond to local motion of the adduct and segmental motion of the polynucleotide, respectively.     

Dimensions in solution of pyridoxylated apohemoglobin

Human apohemoglobin was labeled at Val-beta 1 with pyridoxamine 5'-phosphate. Correlation times were evaluated from steady-state fluorescence anisotropy and lifetime measurements upon quenching with KI. Multiple correlation times were present in the system with a major component of 23.3 ns and a minor component of less than 0.1 ns. The initial depolarization produced by these fast motions occurred in a cone with a semiangle near 33 degrees. The sedimentation velocity and circular dichroism spectra of pyridoxal 5'-phosphate labeled apohemoglobin were very similar to those of unlabeled apohemoglobin. Addition of 8-anilino-1-naphthalenesulfonate did not modify these parameters. Energy transfer of fluorescence was measured between the label, pyridoxamine 5'-phosphate, positioned at Val-beta 1, as donor, and 8-anilino-1-naphthalenesulfonate, bound inside the heme pocket, as acceptor. A quantum yield of 0.21 was measured for labeled apohemoglobin with a standard of pyridoxamine 5'-phosphate. Quenching of the lifetime and of the emission of the donor in the presence of acceptor was measured at 390 nm upon excitation at 313 nm. From these parameters, and on assumption of a random orientation of the fluorophores, an average distance of about 25 A was estimated between the two probes. Numerical correction for 85% saturation of the donor with acceptor produced distances near 23 A for the quenching of emission intensity and near 19 A for the quenching of lifetimes. In the tridimensional model of deoxyhemoglobin, the distance between Val-beta 1 and the nearest iron is about 22 A. Transfer to acceptors positioned in the alpha subunits was negligible. Taking into account the dimensions of the probes, it appears that removal of heme and the consequent loss of helical structure of the system did not produce an expansion of the beta subunits.     

Excimer fluorescence of pyrene-tropomyosin adducts

Studies of the fluorescence of N-(1-pyrene)maleimide and N-(1-pyrenyl)iodoacetamide with actin from rabbit skeletal muscle tropomyosin revealed the presence of excimer fluorescence characterized by a broad emission band at 480 nm with a shoulder at 505 nm. Monomer fluorescence decay exhibited different lifetimes, viz., about 3, 22 and 87 ns for the pyrenemaleimide adduct; about 2.5, 11 and 51 ns for the aminolyzed maleimide adduct: and about 2.5, 15 and 74 ns for the pyrenyliodoacetamide adduct. Almost identical excimer fluorescence lifetimes were found for all adducts; about 9, 35 and 65 ns. Excimer fluorescence was sensitive to changes in ionic strength and pH of the medium while monomer fluorescence did not change. The protein denaturants guanidine hydrochloride and urea caused dissociation of the two tropomyosin subunits and partial disappearance of excimer fluorescence, but not as effectively as the hydrophobic surfactant sodium dodecyl sulfate. The sensitivity of excimer fluorescence to changes in the micro-environment make these pyrene derivatives very useful probes for studying conformational changes and binding interaction of tropomyosin with other contractile proteins. The unique location of the excimer probe at tropomyosin Cys-190 and its characteristic long lifetimes could make it useful in time-resolved anisotropy studies and fluorescence energy-transfer experiments.     

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.     

Dynamic fluorescence study of the interaction of lumazine protein with bacterial luciferases

The equilibrium association of lumazine protein from Photobacterium phosphoreum with luciferases from either P. phosphoreum or an aldehyde-requiring dark mutant of Vibrio harveyi is measured from changes of the rotational correlation time which is derived from the decay of the lumazine ligand's fluorescence anisotropy. The rotational correlation time of lumazine protein is 23 ns (2 degrees C, 0.25 M Pi) and is increased on addition of luciferase due to the formation of a higher molecular weight complex. The V. harveyi luciferase exhibits full competence for the association and a 1:1 stoichiometry with a Kd in the range 40-90 microM. At lower ionic strength (0.05 M Pi), the Kd increases but is reduced again by the addition of dodecanol or dimyristoyllecithin. In contrast, tetradecanal, a substrate for the bioluminescence reaction, exerts no influence on the association. The equilibration rate is found to be too slow and for both luciferases the Kd values are too high for the interaction of the native proteins to account quantitatively for the spectral shifting of the bioluminescence by lumazine protein.     

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.     

Fluorescence characteristics of 5-carboxytetramethylrhodamine linked covalently to the 5'' end of oligonucleotides: multiple conformers of single-stranded and double-stranded dye-DNA complexes.

Fluorescence steady-state and lifetime experiments have been carried out on duplex and single-stranded DNA molecules labeled at the 5' ends with 5-carboxytetramethylrhodamine (TMRh). The temperature and ionic strength of the solutions were varied over large ranges. The results reveal at least three well-defined states of the TMRh-DNA molecules for the single-stranded as well as for the double-stranded DNA molecules. Two states are fluorescent, with lifetimes in the range of 0.5-1 ns and 2.5-3 ns. A third state of TMRh-DNA does not fluoresce (a dark species of TMRh-DNA). The distribution of the TMRh-DNA molecules among these three states is strongly temperature and ionic strength dependent. Estimates are made of some reaction parameters of the multistate model. The results are discussed in terms of the photophysics of TMRh, and consequences of the multiple conformers of TMRh-DNA for studies involving fluorescence studies with TMRh-labeled DNA are considered.     

Fluorescence polarization study of the alpha-ketoglutarate dehydrogenase complex from Escherichia coli

The lipoic acids of the alpha-ketoglutarate dehydrogenase multienzyme complex from Escherichia coli have been modified with two fluorescent probes, N-(1-pyrenyl)-maleimide and 5-[[[(iodoacetyl)amino]ethyl]amino]-naphthylene-1-sulfonic acid. Time-resolved fluorescence polarization of partially labeled complexes (18-77% inhibition of enzyme activity) reveals a complex depolarization process: one component of the anisotropy is characterized by a rotational correlation time much longer than the time scale of the measurements (less than or equal to 400 ns), reflecting the overall rotation of the complex, while a second component of the anisotropy decays with a rotational correlation time of 320 (+/- 50) ns. This decay is essentially independent of viscosity and is consistent with a model in which the depolarization is due to the dissociation from and rotation of lipoic acids between binding sites on the multienzyme complex. The sum of the rate constants characterizing the association and dissociation with the binding sites is approximately 3 x 10(6) s-1. In addition, approximately 5% of the anisotropy of the N-(1-pyrenyl)maleimide-labeled complex decays with a rotational correlation time of 25 ns; this can be attributed to local motion of the probe. At high extents of N-(1-pyrenyl)maleimide labeling (90-95% inhibition of enzyme activity), the anisotropy decay can be described by a constant term plus a rotational correlation time of about 1 microseconds. The increase in the correlation time probably reflects interactions between pyrene moieties. The N-(1-pyrenyl)maleimide-labeled dihydrolipoyl transsuccinylase core of the multienzyme complex has been isolated, and the anisotropy is constant over the observed time range of 300 ns. This suggests that the native structure is necessary for observation of lipoic acid movement within the complex. Fluorescent-labeled limited trypsin digestion fragments of the alpha-ketoglutarate dehydrogenase complex also have been isolated, and anisotropy measurements reveal substantial mobility of the label within the fragments. The time-resolved anisotropy of FAD in the native complex and in the isolated dihydrolipoyl dehydrogenase indicates some rapid local mobility of the FAD (rotational correlation time of 12 ns) that is viscosity independent, as well as a component of the anisotropy that is constant over the 35-ns time scale of the experiments.     

The 2'-O- and 3'-O-Cy3-EDA-ATP(ADP) complexes with myosin subfragment-1 are spectroscopically distinct

Ribose-modified highly-fluorescent sulfoindocyanine ATP and ADP analogs, 2'(3')-O-Cy3-EDA-AT(D)P, with kinetics similar to AT(D)P, enable myosin and actomyosin ATPase enzymology with single substrate molecules. Stopped-flow studies recording both fluorescence and anisotropy during binding to skeletal muscle myosin subfragment-1 (S1) and subsequent single-turnover decay of steady-state intermediates showed that on complex formation, 2'-O- isomer fluorescence quenched by 5%, anisotropy increased from 0.208 to 0.357, and then decayed with turnover rate k(cat) 0.07 s(-1); however, 3'-O- isomer fluorescence increased 77%, and anisotropy from 0.202 to 0.389, but k(cat) was 0.03 s(-1). Cy3-EDA-ADP.S1 complexes with vanadate (V(i)) were studied kinetically and by time-resolved fluorometry as stable analogs of the steady-state intermediates. Upon formation of the 3'-O-Cy3-EDA-ADP.S1.V(i) complex fluorescence doubled and anisotropy increased to 0.372; for the 2'-O- isomer, anisotropy increased to 0.343 but fluorescence only 6%. Average fluorescent lifetimes of 2'-O- and 3'-O-Cy3-EDA-ADP.S1.V(i) complexes, 0.9 and 1.85 ns, compare with approximately 0.7 ns for free analogs. Dynamic polarization shows rotational correlation times higher than 100 ns for both Cy3-EDA-ADP.S1.V(i) complexes, but the 2'-O-isomer only has also a 0.2-ns component. Thus, when bound, 3'-O-Cy3-EDA-ADP's fluorescence is twofold brighter with motion more restricted and turnover slower than the 2'-O-isomer; these data are relevant for applications of these analogs in single molecule studies.     

Time-resolved fluorescence studies on the ternary complex formed between bacterial elongation factor Tu, guanosine 5'-triphosphate, and phenylalanyl-tRNAPhe

Time-resolved fluorescence spectroscopy was used to investigate the solution dynamics of Escherichia coli tRNAPhe, Phe-tRNAPhe, and Phe-tRNAPhe associated with GTP and elongation factor Tu (EF-Tu) in a ternary complex. Two fluorescence probes were employed: fluorescein, covalently bound to Phe-tRNAPhe at the s4U8 base (Phe-tRNAPhe-Fl8), and ethidium bromide, noncovalently associated with the tRNA (EB.Phe-tRNAPhe). The lifetimes observed for ethidium bromide were 1.89 ns, free in solution, and 26.3 ns, bound to its tight binding site on tRNA. Fluorescein-labeled tRNA had a lifetime of 4.3 ns, with no significant difference among the values for aminoacylated, unacylated, and EF-Tu-bound Phe-tRNAPhe-Fl8. Differential phase and modulation data for each fluorophore-tRNA system were fit with local and global Debye rotational relaxation times. Local motion of the labeled fluorescein in Phe-tRNAPhe-Fl8, tRNAPhe-Fl8, and Phe-tRNAPhe-Fl8.EF-Tu.GTP was characterized by rotational relaxation times of 2.7 +/- 0.5, 2.4 +/- 0.4, and 2.4 +/- 0.1 ns, respectively. These values are equal, within experimental error, and suggest that the rotational mobility of the s4U8-conjugated dye is unaffected by either tRNAPhe aminoacylation or ternary complex formation. Global rotational relaxation times for Phe-tRNAPhe-Fl8, 97 ns, and EB.Phe-tRNAPhe, 140 ns, were equivalent to those determined for the unacylated species, denoting little change in the overall size or shape of the tRNA molecule upon aminoacylation. These values for (Phe-)tRNA were larger than expected for a hydrated sphere of equivalent volume, 83 ns, and therefore confirm the asymmetric nature of the tRNA structure in solution.(ABSTRACT TRUNCATED AT 250 WORDS)     

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

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

Characterization of the tryptophan environments of interleukins 1 alpha and 1 beta by fluorescence quenching and lifetime measurements

The tryptophan environments of interleukins 1 alpha and 1 beta, immunomodulatory proteins with similar biological activities but only 25% sequence homology, were characterized by steady-state and dynamic fluorescence measurements. Both proteins exhibited similar emission maxima, but the emission intensity of IL-1 beta was greatly enhanced by increasing the ionic strength of the medium, whereas that of IL-1 alpha was unaffected. The two cytokines were also similarly quenched by the polar quencher acrylamide, but differences were observed for the ionic quenchers iodide and cesium. The fluorescence intensity decays of both cytokines were characterized by two (long and short) component lifetimes. However, the average lifetime of IL-1 beta (4.4 ns) was much longer than that of IL-1 alpha (1.93 ns). Taken together with the results of steady-state measurements, we suggest that the single tryptophan of IL-1 beta is statically quenched by neighboring charged residues, whereas the tryptophan fluorescence of IL-1 alpha is unaffected by ionic strength, and that the tryptophans of the two proteins have different accessibilities to ionic quenchers. The results are discussed in terms of similarities and differences in the tryptophan environments of the two proteins.     

Ligand-induced myosin subfragment 1 global conformational change

The effects of selected ligands on the structure of myosin subfragment 1 (S1) were compared by using transient electrical birefringence techniques. With pairs of dilute solutions of S1 at 3.5 degrees C in low ionic strength (mu = 0.020 M) buffers that had matched electrical impedances, S1 with Mg2+, MgADP, or MgADP.Vi bound was subjected to 6-7-microseconds external electrical fields in the Kerr law range. Specific Kerr constants and the rates of rotational Brownian motion after the electric field was removed were measured. Neither Mg2+ nor MgADP had a measurable effect on either observable, but when orthovanadate (Vi) bound S1.MgADP it decreased the rotational correlation coefficient from 267 +/- 6 to 244 +/- 10 ns. Parallel measurements of MgATPase activity indicated that S1.MgADP.Vi was greater than 95% inhibited. These results confirm the conclusion of Aguirre et al. [(1989) Biochemistry 28, 799] that Vi binding to S1.MgADP increases its rate of rotational Brownian motion and provide data that are more quantitatively correlated with S1 structure. The Vi-induced change in the rotational correlation coefficient is consistent with S1 becoming more flexible or more compact when Vi binds. Assuming that S1.MgADP.Vi is an analogue for S1.MgADP.Pi, the structural changes observed for S1-ligand complexes in solution are discussed in relation to possible structural changes of intermediates on the kinetic pathway of ATPase hydrolysis. A new model of force generation by S1 in muscle is hypothesized.     

Fluorescence studies on the interactions of myelin basic protein in electrolyte solutions.

This paper examines the influence of electrolytes on fluorescence spectral properties of the single tryptophanyl residue, Trp-115, within the 18.5-kDa species of myelin basic protein from bovine brain. Steady-state fluorescence spectra and intensities and time-correlated fluorescence lifetimes increased in the presence of increasing concentrations of mono- and divalent electrolytes (Li+, Na+, K+, Mg2+, Ca2+, Cl-, ClO4-, SO4(2-), and PO4(3-)). In all cases, the increases closely paralleled the ionic strength of the bulk aqueous medium and resembled that observed upon immersion of the protein in solutions of urea. This behavior was therefore concluded to reflect changes in the solution conformation of myelin basic protein. Bimolecular quenching of Trp-115 by acrylamide was rapid (10(9) M-1 s-1), approaching the diffusion limitation, and markedly dependent on the viscosity of the bulk aqueous medium. Rotational depolarization of myelin basic protein was rapid (phi less than or equal to 1 ns), occurring at rates exceeding those predicted for a rigid particle of revolution, and markedly dependent on the viscosity of the surrounding medium. Whereas the bimolecular quenching constants were unaltered in the presence of electrolytes, rotational depolarization of myelin basic protein underwent substantial slowing as indicated by the appearance of an additional decay component characterized by a correlation time of 5-10 ns. These studies indicate that Trp-115 of myelin basic protein is readily accessible to the bulk aqueous medium and is associated with a highly mobile segment of the protein. The slowing of rotational depolarization upon immersion of myelin basic protein in electrolyte solutions is consistent with an electrolyte-induced self-association of myelin basic protein molecules and indicates a relationship between the lability of solution conformation on the one hand and the capacity for self-association on the other.     

A time-resolved fluorescence study of 4',6'-diamidine-2-phenylindole dihydrochloride binding to polynucleotides

At phosphate/dye (P/D) ratios greater than 30 the quantum yield of 4',6'-diamidine-2-phenylindole dihydrochloride (DAPI)-DNA and DAPI-poly(d(A-T)) complexes was found to be 0.62 and 0.66, respectively. Contrary to earlier reports a fluorescence enhancement of DAPI-poly(d(G-C)) complexes was observed with a quantum yield of 0.22. Time-resolved fluorescence measurements of complexes with a P/D ratio of 150:1 indicate that there were three fluorescent components in DAPI-DNA complexes with lifetimes of 3.86, 1.79 and 0.13 ns. In DAPI-poly(d(A-T)) complexes the lifetimes were 3.91, 1.20 and 0.11 ns. Also, three components with lifetimes of 3.98, 0.87 and 0.12 ns were found in DAPI-poly(d(G-C)) complexes. At low P/D ratios (< 5) another binding form of DAPI was observed which was assigned to the interaction of one or more molecules of DAPI with one previously bound to DNA. It is concluded that DAPI does not exhibit A-T binding specificity and that at high P/D ratios there are two types of binding having similar binding constants.