Chromatic shifts in the fluorescence emitted by murine thymocytes stained with Hoechst 33342.

BACKGROUND: Many methods in flow cytometry rely on staining DNA with a fluorescent dye to gauge DNA content. From the relative intensity of the fluorescence signature, one can then infer position in cell cycle, amount of DNA (i.e., for sperm selection), or, as in the case of flow karyotyping, to distinguish individual chromosomes. This work examines the staining of murine thymocytes with a common DNA dye, Hoechst 33342, to investigate nonlinearities in the florescence intensity as well as chromatic shifts. METHODS: Murine thymocytes were stained with Hoechst 33342 and measured in a flow cytometer at two fluorescence emission bands. In other measurements, cells were stained at different dye concentrations, and then centrifuged. The supernatant was then used for a second round of staining to test the amount of dye uptake. Finally, to test for resonant energy transfer, we measured fluorescence anisotropy at two different wavelengths. RESULTS: The fluorescence of cells stained with Hoechst 33342 is a nonlinear process that shows an overall decrease in intensity with increased dye uptake, and spectral shift to the red. Along with the spectral shift of the fluorescence to the longer wavelengths, we document decreases in the fluorescence anisotropy that may indicate resonant energy transfer. CONCLUSIONS: At low concentrations, Hoechst 33342 binds to the minor groove of DNA and shows an increase in fluorescence and a blue shift upon binding. At higher concentrations, at which the dye molecules can no longer bind without overlapping, the blue fluorescence decreases and the red fluorescence increases until there is approximately one dye molecule per DNA base pair. The ratio of the blue fluorescence to the red fluorescence is an accurate indicator of the cellular dye concentration.     

Dynamics of drug-DNA interactions: a comparative temperature jump study of ellipticinium and 9-hydroxy ellipticinium

The temperature-jump method has been used to compare the binding of 2-N methyl ellipticinium (NME) and 2-N methyl 9 hydroxy ellipticinium (NMHE) to three natural DNA's of different AT/GC composition. The relaxation signals, analyzed by the Padé-Laplace method, are characterized by two distinct relaxation times, tau 1 and tau 2, respectively in the 1-4 ms and 20-80 ms range. In the case of the NMHE/DNA interaction, the slower relaxation time tau 2 depends on the DNA composition, as follows: tau 2 (Micrococcus lysodeikticus) greater than tau 2 (Calf thymus) greater than tau 2 (Clostridium perfringens). Contrary to NMHE, NME which does not possess an OH group at the C-9 position, shows no relaxation time dependence upon DNA base composition. The observation of two relaxation times indicates that the binding equilibria are associated with at least two distinct drug/DNA complexes (probably arising from two distinct DNA binding sites). Three kinetic models, involving the formation of a weak intermediate ionic complex, are given to explain the binding reaction between these cationic drugs and the DNA. They allow the determination of the four rate constants associated with the two binding steps and lead to equilibrium association constants in agreement with those obtained from spectroscopic studies. The validity of the models is discussed and it is shown that the best kinetic scheme, for either NMHE or NME, could be that in which the ionic step is not a prerequiste to intercalation. The kinetic results show that the residence time of 9 hydroxy ellipticinium is markedly increased in GC rich DNA's and this could be related to the higher in vitro and in vivo cytotoxic properties of 9 hydroxy substituted ellipticines.     

DNA-ethidium reaction kinetics: demonstration of direct ligand transfer between DNA binding sites.

Study of the relaxation kinetics of the interaction of ethidium and DNA reveals a novel and potentially important general binding mechanism, namely direct transfer of the ligand between DNA binding sites without requiring dissociation to free ligand. The measurable relaxation spectrum shows three relaxation times, indicating that three bound dye species are present at equilibrium; about 80% of the dye is in the major intercalated form. For each relaxation the reciprocal relaxation time varies linearly with concentration up to very high DNA concentrations. The failure of the longer relaxation times to plateau at high concentration can be accounted for by including a bimolecular pathway for conversion from one complex form to another. This we envisage as direct transfer of an ethidium molecule, bound to one DNA molecule, to an empty binding site on another DNA molecule. Additional evidence for this direct transfer mechanism was obtained from an experiment showing that DNA (which binds ethidium relatively rapidly) accelerates the binding of ethidium to poly(rA) · poly(rU), presumably by first forming a DNA-ethidium complex and then transferring the ethidium to RNA. The bimolecular rate constant for transfer is found to be about four times larger than the constant for intercalating the free dye. The transfer pathway thus provides a highly efficient means for the ligand to equilibrate over its DNA binding sites, especially at high polymer concentration. The potential importance of direct transfer for DNA-binding regulatory proteins is emphasized.     

Study of propidium iodide binding to DNA in intact cells by flow cytometry.

We studied the in situ binding of propidium iodide to DNA in fixed human lymphocytes, using flow cytometry. Experimental data of fluorescence emission vs dye concentration and vs cell concentration were obtained. Data were interpreted by means of two different mathematical models specific for the staining reaction, and the binding parameters were obtained by "best-fitting" of the data. A model based on two classes of binding sites with different affinity constants gave the most satisfactory fitting. The accessibility of the in situ chromatin turned out to be reduced with respect to the non in situ accessibility for ethidium bromide as reported in the literature. The present study shows the usefulness of the flow-cytometric technique for probing DNA structure in intact cells.     

Proflavin binding to poly[d(A-T)] and poly[d(A-br5U)]: triplet state and temperature-jump kinetics

The delayed fluorescence properties of proflavin have been exploited in studies of the excited-state binding kinetics of the dye to poly[d(A-T)] and its brominated analogue poly[d(A-br5U)] at room temperature and pH 7. The two analyzed luminescence decay times of the DNA-dye complex are dependent on the total nucleic acid concentration. This dependence is shown to reflect a temporal coupling of the intrinsic delayed emission decay rates with the dynamic chemical kinetic binding processes in the excited state. Temperature-jump kinetic studies conducted on the brominated polymer and corresponding information on poly[d(A-T)] from a previous study [Ramstein, J., Ehrenberg, M., & Rigler, R. (1980) Biochemistry 19, 3938-3948] provide complementary information about the ground state. In the ground state, the poly[d(A-T)]-proflavin complex has one chemical relaxation time, which reaches a plateau at high DNA concentrations. The brominated DNA-dye complex exhibits two relaxation times: a faster relaxation mode that behaves similarly to that for the unhalogenated DNA and a slower relaxation mode that is apparent at high DNA concentrations. The ground-state kinetic data are analyzed in terms of two alternative models incorporating series and parallel reaction schemes. The former consists of two sequential binding steps--a fast bimolecular process followed by a monomolecular step--while the latter consists of two coupled bimolecular steps. A similar analysis for the excited-state data yields reasonable kinetic constants only for the series model, which, in accordance with previous proposals for acridine intercalators, consists of a fast outside binding step followed by intercalation of the dye. A comparison of the ground- and excited-state kinetic parameters reveals that the external binding process is much stronger and the intercalation is much weaker in the excited state. That the excited-state data are only consistent with the series model suggests that delayed luminescence studies may provide a general tool for distinguishing between the two kinetic mechanisms. In particular, we demonstrate the use of delayed luminescence spectroscopy as a tool for probing dynamic DNA-ligand interactions in solution.     

The reaction of aromatic peptides with double helical DNA. Quantitative characterisation of a two step reaction scheme

The binding of LysTrpLys and LysTyrLys to calf thymus DNA has been investigated by the field jump method using fluorescence detection. Two separate relaxation processes, clearly distinguished on the time scale and by opposite ampli- tudes, are observed for the binding of LysTrpLys to DNA with ~ 30000 base pairs. The concentration dependence of the relaxation time constants demonstrates a mechanism with a bimolecular step followed by a slow intramolecular transition with a forward rate of 6.4 X 103 s^?1 and an equilibrium constant of 11. Measurements at various degrees of peptide binding demonstrate that the binding mechanism associated with low binding rates is restricted to a rather low number of binding sites (roughly one site in 15 base pairs). The binding of LysTyrLys to the same DNA is not associated with relaxation pro- cesses of opposite amplitudes; nevertheless two processes could be identified and assigned to a two step mechanism corre- sponding to that observed in the case of LysTrpLys. In the presence of sonicated DNA both peptides show a single relaxa- tion process with characteristics similar to those observed for the slow process in the binding to high molecular DNA. The data indicate that the intramolecular step is faster for low than for high molecular DNA. These results suggest an assignment of the intramolecular step to an insertion of the aromatic residues into the DNA associated with bending of the helix. The increase in the rate of the intramolecular step with decreasing chain length of the DNA may then be explained by a higher flexibility of the double helix at lower chain lengths.     

Spectral manifestations of different types of acriflavine binding to DNA in ultraviolet and visible region]

Difference absorption spectra (complex-sum of the initial reagents) are obtained in the visible and longwave UV region for the system of actiflavine and DNA in a number of cases differing in initial and final degrees of DNA filling by the dye, in particular separately for two types of dye binding to DNA. For these binding types conventional absorption spectra are calculated. In the visible region for the first binding type ("strong" binding) red shift of the absorption band is observed; for the second type ("weak" binding) we observed splitting of the band, short wavelength component being highly prevailing, and hypochromism. In the UV region for both binding types the spectra changed in approximately similar way; a slight blue shift and a rather remarkable hypochromism are observed. It is shown that the dye brings the main contribution into the spectral changes in the UV region. If to take into account the spectral properties of molecular aggregates the data obtained are compatible with the intercalation model for "strong" binding and dye stacking on DNA for "weak" binding.     

Kinetics of the daunomycin--DNA interaction

The kinetics of the interaction of daunomycin with calf thymus DNA are described. Stopped-flow and temperature-jump relaxation methods, using absorption detection, were used to study the binding reaction. Three relaxation times were observed, all of which are concentration dependent, although the two slower relaxations approach constant values at high reactant concentrations. Relaxation times over a wide range of concentrations were gathered, and the data were fit by a minimal mechanism in which a rapid bimolecular association step is followed by two sequential isomerization steps. The six rate constants for this mechanism were extracted from our data by relaxation analysis. The values determined for the six rate constants may be combined to calculate an overall equilibrium constant that is in excellent agreement with that obtained by independent equilibrium measurements. Additional stopped-flow experiments, using first sodium dodecyl sulfate to dissociate bound drug and second pseudo-first-order conditions to study the fast bimolecular step, provide independent verification of three of the six rate constants. The temperature dependence of four of the six rate constants was measured, allowing estimates of the activation energy of some of the steps to be made. We speculate that the three steps in the proposed mechanism may correspond to a rapid "outside" binding of daunomycin to DNA, followed by intercalation of the drug, followed by either conformational adjustment of the drug or DNA binding site or redistribution of bound drug to preferred sites.     

The binding of 4',6-diamidino-2-phenylindole to bovine serum albumin.

The binding of 4',6-diamidino-2-phenylindole (DAPI) to bovine serum albumin (BSA) has been investigated between pH 6 and 8, in 0.05 M phosphate buffer at 20 degrees C, by fluorescence titrations and the results analyzed according to a procedure previously reported (R. Favilla and A. Mazzini, Biochim. Biophys. Acta 788 (1984) 48). The dye binds to the protein with a blue shift of about 4 nm in its fluorescence emission maximum, but with an enhancement factor of 10 of its fluorescence quantum yield. The dissociation constant decreases from 100 microM to 54 microM as the pH is increased from 6 to 8, with a constant number of nearly three equivalent binding sites. The complete displacement of DAPI bound to BSA by Ca2+ suggests a possible specificity of this substantially electrostatic interaction. The fluorescence decay of DAPI bound to the protein shows a double exponential kinetics, with a tau 1 = 0.97 ns and tau 2 = 2.78 ns. These results, compared with those obtained for DAPI alone, tau 1 = 0.16 ns and tau 2 = 2.8 ns, are rationalized in terms of two different rotamers of DAPI. Both rotamers are able to bind to the protein, but only one of them undergoes an intramolecular proton transfer, from the 6-amidinium group to the indole aromatic ring, in the excited singlet state of DAPI alone. When DAPI interacts with BSA this transfer does not occur and consequently a large increase of fluorescence is observed.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fluorescence decay studies of the DNA-3,6-diaminoacridine complexes

The interaction of several 3,6-diaminoacridines with DNAs of various base composition has been studied by steady-state and transient fluorescence measurements. The acridine dyes employed are of the following two classes: class I - proflavine, acriflavine and 10-benzyl proflavine; class II - acridine yellow, 10-methyl acridine yellow and benzoflavine. It is found that the fluorescence decay kinetics follows a single-exponential decay law for free dye and the poly[d(A-T)]-dye complex, while that of the dye bound to DNA obeys a two-exponential decay law. The long lifetime (tau 1) for each complex is almost the same as the lifetime for the poly[d(A-T)]-dye complex, and the amplitude alpha 1 decreases with increasing GC content of DNA. The fluorescence quantum yields (phi F) of dye upon binding to DNA decrease with increasing GC content; the phi F values for class I are nearly zero when bound to poly(dG) X poly(dC), but those for class II are not zero. This is in harmony with the finding that GMP almost completely quenches the fluorescence for class I, whereas a weak fluorescence arises from the GMP-dye complex for class II. The fluorescence spectra of the DNA-dye complexes gradually shift toward longer wavelengths with increasing GC content. In this connection, the fluorescence decay parameters show a dependence on the emission wavelength; alpha 1 decreases with an increase in the emission wavelength. In view of these results, it is proposed that the decay behavior of the DNA-dye complexes has its origin in the heterogeneity of the emitting sites; the long lifetime tau 1 results from the dye bound to AT-AT sites, while the short lifetime tau 2 is attributable to the dye bound in the vicinity of GC pairs. Since GC pairs almost completely quench the fluorescence for class I, partly intercalated or externally bound dye molecules may play an important role in the component tau 2.     

Relaxation phenomena in human erythrocyte suspensions.

Previous work has shown that the application of the Joule heating temperature jump technique of Eigen and de Maeyer to an istonic suspension of human erythrocytes induced an interiorization of [3H-A1glucose and a hemolysis of the red cells (Tsong, T.Y., and E. Kingsley, J. Biol. Chem. 250:786 [1975]). The result was interpreted as due to the thermal osmosis effect. Further considerations of the various effects of the Joule heating technique indicate that the hemolysis of the red cells may also be caused by the rapid dielectric perturbation of the cell membranes. By means of turbidity measurements of the suspensions we have detected at least four relaxation times. Two of the faster ones (tau1 approximately 20 mus and tau2 approximately 5 ms) are tentatively attributed to water relaxations in the membrane structures. The other two are attributed to membrane ruptures (tlag approximately 0.1s) and the hemolysis reaction (tau3 approximately 0.5 s). Studies with the erythrocytes from different hematological disorders indicate that whereas the two slower relaxations are sensitive to the overall physical property of the red cell membranes the two faster relaxations are not. These observations are consistent with the above assignment of the relaxation processes. The apparent activation energies are, above assignment of the relaxation processes. The apparent activation energies are, respectively, 8.4, 12.0, and 11.8 kcal/mol for the tau1, tau2, and tau3 reactions. Experiments with erythrocyte ghosts indicate a single relaxation for the water permeation, and biphasic kinetics for the membrane rupture and resealing reactions. The phenomena reported here may contribute to our understanding of water transport and molecular release in cellular systems.     

Simultaneous DNA binding, bending, and base flipping: evidence for a novel M.EcoRI methyltransferase-DNA complex

We measured the kinetics of DNA bending by M.EcoRI using DNA labeled at both 5'-ends and observed changes in fluorescence resonance energy transfer. Although known to bend its cognate DNA site, energy transfer is decreased upon enzyme binding. This unanticipated effect is shown to be robust because we observe the identical decrease with different dye pairs, when the dye pairs are placed on the respective 3'-ends, the effect is cofactor- and protein-dependent, and the effect is observed with duplexes ranging from 14 through 17 base pairs. The same labeled DNA shows the anticipated increased energy transfer with EcoRV endonuclease, which also bends this sequence, and no change in energy transfer with EcoRI endonuclease, which leaves this sequence unbent. We interpret these results as evidence for an increased end-to-end distance resulting from M.EcoRI binding, mediated by a mechanism novel for DNA methyltransferases, combining DNA bending and an overall expansion of the DNA duplex. The M.EcoRI protein sequence is poorly accommodated into well defined classes of DNA methyltransferases, both at the level of individual motifs and overall alignment. Interestingly, M.EcoRI has an intercalation motif observed in the FPG DNA glycosylase family of repair enzymes. Enzyme-dependent changes in anisotropy and fluorescence resonance energy transfer have similar rate constants, which are similar to the previously determined rate constant for base flipping; thus, the three processes are nearly coincidental. Similar fluorescence resonance energy transfer experiments following AdoMet-dependent catalysis show that the unbending transition determines the steady state product release kinetics.     

N-(5-Phosphoribosyl)anthranilate isomerase-indoleglycerol-phosphate synthase. 2. Fast-reaction studies show that a fluorescent substrate analogue binds independently to two different sites.

The mechanism of binding of reduced 1-(2-carboxyphenylamino)-1-deoxyribulose 5-phosphate (rCdRP) to two different binding sites on the bifunctional enzyme is determined by kinetic studies, using temperature-jump and stopped-flow equipment with fluorescence detection. Two rapid binding processes and a comparatively slow isomerization process are observed over a wide range of enzyme and rCdRP concentrations. Kinetic measurements with low concentrations of rCdRP show that the isomerization is coupled only to the more rapid of the two binding reactions that involves the active site of indoleglycerol-phosphate synthase. The slower of the two binding reactions represents rCdRP binding in one step to the active site of (phosphoribosyl)anthranilate isomerase. The simplest mechanism explaining quantitatively the dependence of the relaxation times on concentration consists of rCdRP binding to two sites on the enzyme that are intrinsically different and independent, even to the extent that a ligand-induced isomerization of one site is not transmitted to the other site. Simulation studies show that the concentration dependences of the amplitudes of the three relaxation processes are also consistent with the mechanism. The results are discussed in terms of two autonomous domains of folding of the polypeptide chain.     

The effect of the medium on the functional and structural properties of serum albumins. III. Relation between the N-F1-, F1-F2- and F2-E transitions of human serum albumin and temperature and ionic strength

Using fluorescence parameters of tryptophanyl and bound ANS, the acid-induced structural transitions of defatted monomeric human serum albumin were measured as pH-dependences from 6 to 2.5 in the wide range of temperature (10 to 45 degrees C) and ionic strength (from 0.001 to 0.2 M NaCl or 0.067 M Na2SO4). Temperature rise and decrease in ionic strength value result in the splitting of the N-F-transition onto two stages, N-F1 and F1-F2. The N-F1-transition is accompanied by the blue shift of tryptophanyl and ANS fluorescence spectra and increase in the ANS emission yield. The F1-F2-stage is manifested in an additional blue spectral shift and a sharp drop of the ANS emission yield, which is shown to be due to the lowering of albumin affinity for the dye. In the acidic-extension stage (F2-E), the spectra undergo a red shift which means that the nanosecond dipole relaxation of protein groups and bound water becomes faster. In the F2 from, the albumin affinity for ANS is significantly lowered; the association constant of the primary binding site is lower by an order of quantity and two secondary sites are practically disappeared. The complex effect of temperature, ionic strength and pH changes on the properties of ANS-binding sites is considered as a model of possible control influences of these factors upon the albumin transport of amphiphilic anions in organism.     

Energy transfer and trapping in the photosystem I core antenna. A temperature study.

The fluorescence decay kinetics of the photosystem I-only mutant strain of Chlamydomonas reinhardtii, A4d, are used to study energy transfer and structural organization in photosystem I (PSI). Time-resolved measurements over a wide temperature range (36-295 K) have been made both on cells containing approximately 65 core chl a/P700 and an additional 60-70 chl a + b from LHC proteins and on PSI particles containing 40-50 chl a/P700. In each case, the fluorescence decay kinetics is dominated by a short component, tau 1 which is largely attributed to the lifetime of the excitations in the core complex. The results are discussed in terms of simulations of the temperature dependence of tau 1 in model systems. Spectral inhomogeneity and the temperature dependence of the spectral lineshapes are included explicitly in the simulations. Various kinds of antenna arrangements are modeled with and without the inclusion of pigments with lower absorption energies than the trap (red pigments). We conclude that funnel arrangements are not consistent with our measurements. A random model that includes one or two red pigments placed close to the trap shows temperature and wavelength dependence similar to that observed experimentally. A comparison of the temperature dependence of tau 1 for cells and PSI particles is included.     

Fast voltage clamp discloses a new component of presteady-state currents from the Na(+)-glucose cotransporter.

The human Na(+)-glucose cotransporter (hSGLT1) has been shown to generate, in the absence of sugar, presteady-state currents in response to a change in potential, which could be fitted with single exponentials once the voltage had reached a new constant value. By the cut-open oocyte technique (voltage rising-speed approximately 1 mV/microsecond), phlorizin-sensitive transient currents could be detected with a higher time resolution during continuous intracellular perfusion. In the absence of sugar and internal Na+, and with 90 mM external Na+ concentration ([Na+]o), phlorizin-sensitive currents exhibited two relaxation time-constants: tau 1 increased from 2 to 10 ms when Vm decreased from +60 mV to -80 mV and remained at 10 ms for more negative Vm; tau 2 ranged from 0.4 to 0.8 ms in a weakly voltage-dependent manner. According to a previously proposed model, these two time constants could be accounted for by 1) Na+ crossing a fraction of the membrane electrical field to reach its binding site on the carrier and 2) conformational change of the free carrier. To test this hypothesis, the time constants were measured as [Na+]o was progressively reduced to 0 mM. At 30 and 10 mM external Na+, tau 1 reached the same plateau value of 10 ms but at more negative potentials (-120 and -160 mV, respectively). Contrary to the prediction of the model, two time constants continued to be detected in the bilateral absence of Na+ (at pH 8.0). Under these conditions, tau 1 continuously increased through the whole voltage range and did not reach the 10 ms level even when Vm had attained -200 mV while tau 2 remained in the range of 0.4-0.8 ms. These results indicate that 1) conformational change of the free carrier across the membrane must occur in more than one step and 2) Na+ binding/debinding is not responsible for either of the two observed exponential components of transient currents. By use of the simplest kinetic model accounting for the portion of the hSGLT1 transport cycle involving extracellular Na+ binding/debinding and the dual-step conformational change of the free carrier, tau 1 and tau 2 were fitted throughout the voltage range, and a few sets of parameters were found to reproduce the data satisfactorily. This study shows that 1) tau 1 and tau 2 correspond to two steps in the conformational change of the free carrier, 2) Na+ binding/debinding modulates the slow time constant (tau 1) and 3) a voltage-independent slow conformational change of the free carrier accounts for the observed plateau value of 10 ms.     

Binding of Hoechst 33258 to chromatin in situ

The binding of Hoechst 33258 to rat thymocytes, human lymphocytes, and NHIK 3025 tissue culture cells was studied by measuring the fluorescence and light scattering of the cells as functions of dye concentration using flow cytometry. The results indicated that there were two different modes of binding of Hoechst 33258 to chromatin in situ at physiological pH. Type 1 binding, which dominated at total dye/phosphate ratios below 0.1 (0.15, M), was characterized by a binding constant of the order 10(7) M-1 and fluorescence with high quantum yield. Further binding of the dye resulted in a reduced blue/green fluorescence ratio, indicating that secondary sites were occupied. Binding at secondary sites above a certain density (0.1 less than or equal to bound dye/phosphate less than or equal to 0.2) induced strong quenching of fluorescence and precipitation of chromatin. Precipitation was quantitated by measuring the large-angle (greater than or equal to 15 degrees) light scattering of the cells above 400 nm, i.e., outside the Hoechst 33258/DNA absorption spectrum, as a function of dye concentration. In contrast, the light scattering at 365 nm, i.e., within the absorption spectrum of Hoechst 33258/DNA, was independent of the total dye/phosphate ratio. The coefficient of variation of the light-scattering (greater than or equal to 400 nm) histograms decreased with Hoechst 33258 concentration. Type 2 binding to histone-depleted chromatin was cooperative (Hill-coefficient approximately 2) and the apparent binding constant was 2-3 X 10(5) M-1 as determined from quenching and precipitation data.(ABSTRACT TRUNCATED AT 250 WORDS)     

Conformational equilibria accompanying the electron transfer between cytochrome c (P551) and azurin from Pseudomonas aeruginosa.

The redox reaction between cytochrome c (Cyt c) (P-551) and the blue copper protein azurin, both from Pseudomonas aeruginosa, was studied using the temperature-jump technique. Two relaxation times were observed in a mechanism assumed to involve three equilibria. The fast relaxation time (0.4 less than tau less than 8 ms) was ascribed to the electron exchange step. The slow relaxation time (tau congruent to 37 ms) was assigned to a conformational equilibrium of the reduced azurin that was coupled through the electron exchange step to a faster conformational equilibrium of the oxidized Cyt c (P551). But because the Cyt c (P551) isomerization, being very rapid, was uncoupled from the two slower equilibria, and was assumed to involve no spectral change, the amplitude of its relaxation time (tau congruent to 0.1 ms) would be zero. At 25 degrees C and pH 7.0 the rate constants for the oxidation and reduction of Cyt c (P551) by azurin were 6.1 X 10(6) and 7.8 X 10(6) M-1 s-1, respectively; for the formation and disappearance of the reactive conformational isomer of azurin they were 12 and 17 s-1, respectively. The rates for the Cyt c (P551) isomerization could only be estimated at approximately 10(4) s-1. The thermodynamic parameters of each reaction step were evaluated from the amplitudes of the relaxations and from Eyring plots of the rate constants. Measurements of the overall equilibrium constant showed it to be temperature independent (5-35 degrees C), i.e. deltaHtot = 0. This zero enthalpy change was found to be compatible with the enthalpies calculated for the individual steps. In the electron exchange equilibrium, the values of the activation enthalpies were two to three times higher than the values published for various low molecular weight reagents in their electron exchange with copper proteins, yet the rate of exchange between Cyt c (P551) and azurin was some hundreds of times faster. This was explained in terms of the measured positive or zero entropies of activation that could result from a high level of specificity between the proteins particularly in areas of complementary charges. The mechanism of electron transfer was considered as essentially an outer sphere reaction, of which the rate could be approximated by the Marcus theory.     

13C NMR and fluorescence analysis of tryptophan dynamics in wild-type and two single-Trp variants of Escherichia coli thioredoxin.

The rotational motion of tryptophan side chains in oxidized and reduced wild-type (WT) Escherichia coli thioredoxin and in two single-tryptophan variants of E. coli thioredoxin was studied in solution in the temperature range 20-50 degrees C from 13C-NMR relaxation rate measurements at 75.4 and 125.7 MHz and at 20 degrees C from steady-state and time-resolved trp fluorescence anisotropy measurements. Tryptophan enriched with 13C at the delta 1 and epsilon 3 sites of the indole ring was incorporated into WT thioredoxin and into two single-trp mutants, W31F and W28F, in which trp-28 or trp-31 of WT thioredoxin was replaced, respectively, with phenylalanine. The NMR relaxation data were interpreted using the Lipari and Szabo "model-free" approach (G. Lipari and A. Szabo. 1982. J. Amer. Chem. Soc. 104:4546-4559) with trp steady-state anisotropy data included for the variants at 20 degrees C. Values for the correlation time for the overall rotational motion (tau m) from NMR of oxidized and reduced WT thioredoxin at 35 degrees C agree well with those given by Stone et al. (Stone, M. J., K. Chandrasekhar, A. Holmgren, P. E. Wright, and H. J. Dyson. 1993. Biochemistry. 32:426-435) from 15N NMR relaxation rates, and the dependence of tau m on viscosity and temperature was in accord with the Stokes-Einstein relationship. Order parameters (S2) near 1 were obtained for the trp side chains in the WT proteins even at 50 degrees C. A slight increase in the amplitude of motion (decrease in S2) of trp-31, which is near the protein surface, but not of trp-28, which is partially buried in the protein matrix, was observed in reduced relative to oxidized WT thioredoxin. For trp-28 in W31F, order parameters near 1 (S2 > or = 0.8) at 20 degrees C were found, whereas trp-31 in W28F yielded the smallest order parameters (S2 approximately 0.6) of any of the cases. Analysis of time-resolved anisotropy decays in W28F and W31F yielded S2 values in good agreement with NMR, but gave tau m values about 60% smaller. Generally, values of tau e, the effective correlation time for the internal motion, were < or = 60 ps from NMR, whereas somewhat longer times were obtained from fluorescence. The ability of NMR and fluorescence techniques to detect subnanosecond motions in proteins reliably is examined.