Dynamic site heterogeneity in amorphous maltose and maltitol from spectral heterogeneity in erythrosin B phosphorescence

We have used phosphorescence from erythrosin B (tetraiodofluorescein) dispersed in thin films of either maltose or maltitol to investigate the physical properties of these amorphous pure sugar matrixes. Intensity decays collected as a function of emission wavelength over the range from 640 to 720 nm were analyzed using a stretched exponential kinetic model in which the lifetime (tau) and the stretching exponent (beta) were the physically relevant parameters. The lifetimes varied systematically with emission wavelength in both matrixes. Analysis of the temperature dependence of the lifetime at each wavelength provided an estimate of the activation energy for nonradiative quenching of the triplet state; the activation energy also varied with emission wavelength. In addition, time-resolved emission spectra exhibited a blue shift with time following excitation. These data support a photophysical model in which probes are distributed among sites that vary in terms of overall molecular mobility and in which sites with lower rates of dipolar relaxation also have lower rates of collisional quenching of the erythrosin triplet state. The amorphous matrix of both maltose and maltitol in both the glass and the melt state is thus characterized by dynamic site heterogeneity in which different sites vary in terms of their overall molecular mobility.     

Molecular Mobility and Oxygen Permeability in Amorphous Bovine Serum Albumin Films

We have used phosphorescence from the xanthene probe erythrosin B to characterize the molecular mobility and oxygen permeability as a function of temperature in amorphous solid bovine serum albumin (BSA) films. Analysis of the emission spectrum using a lognormal fitting function provided information on how temperature modulates the emission peak frequency and bandwidth (full width at half maximum). The peak frequency decreased gradually at low and more steeply at high temperature, whereas the bandwidth increased gradually at low and more steeply at high temperature, both changes indicating a softening of the protein matrix at ∼60°C. Phosphorescence intensity decay transients were well fit using a stretched exponential decay function at all temperatures. Lifetimes decreased gradually at low and more steeply at high temperature; Arrhenius analysis of the rate constant for nonradiative collisional quenching indicated an increase in quenching indicative of matrix softening at ∼70°C. The oxygen quenching rate was calculated from a comparison of emission lifetimes in the presence and absence of oxygen. This rate varied linearly with the collisional quenching rate over nearly three orders of magnitude, suggesting that the more global motions that control oxygen translational diffusion are modulated by more local motions that influence collisional quenching of erythrosin. The emission spectrum shifted to higher energy as a function of time following excitation, whereas the phosphorescence lifetime decreased with increasing emission wavelength; both behaviors provided strong evidence for distinct sites within the protein matrix varying in molecular mobility. These results enrich our molecular understanding of the intrinsic mobility of proteins within the amorphous solid phase, provide evidence for a dynamic transition within solid BSA, and provide insight into the molecular mechanisms controlling oxygen diffusion.     

Erythrosin B phosphorescence monitors molecular mobility and dynamic site heterogeneity in amorphous sucrose

Molecular mobility modulates the chemical and physical stability of amorphous biomaterials. This study used steady-state and time-resolved phosphorescence of erythrosin B to monitor mobility in thin films of amorphous solid sucrose as a function of temperature. The phosphorescence intensity (lifetime), emission energy, and red-edge excitation effect were all sensitive to localized molecular mobility on the microsecond timescale in the glass and to more global modes of mobility activated at the glass transition. Blue shifts in the emission spectrum with time after excitation and systematic variations in the phosphorescence lifetime with wavelength indicated that emission originates from multiple sites ranging from short lifetime species with red-shifted emission spectrum to long lifetime species with blue-shifted emission spectrum; the activation energy for nonradiative decay of the triplet state was considerably larger for the blue-emitting species in both the glass and the melt. This study illustrates that phosphorescence from erythrosin B is sensitive both to local dipolar relaxations in the glass as well as more global relaxations in the sucrose melt and provides evidence of the value of phosphorescence as a probe of dynamic site heterogeneity as well as overall molecular mobility in amorphous biomaterials.     

Effect of gelatin on molecular mobility in amorphous sucrose detected by erythrosin B phosphorescence

We have used phosphorescence from the triplet probe erythrosin B (Ery B) to evaluate the effect of gelatin on the molecular mobility of the amorphous sucrose matrix as a function of temperature. Ery B was dispersed in amorphous sucrose and sucrose-gelatin films at ratios of approximately 1:10(4) (probe/sucrose), and delayed emission spectra and emission decay transients were measured over the temperature range from 5 to 100 degrees C. Analysis of spectra using a lognormal function provided the peak energy and bandwidth of the emission. The emission peak frequency decreased at low (0.00022-0.0007) gelatin concentrations and increased at high (above 0.0022) gelatin concentrations, indicating that gelatin increased the extent, and thus the rate, of dipolar relaxation at low gelatin content and decreased the extent at higher gelatin content. Decay transients were well fit to a stretched exponential function at all gelatin contents and temperatures. Analysis of the emission lifetimes provided a measure of the rate of non-radiative decay to the ground state, an indicator of matrix molecular mobility. This rate increased at low (0.00022-0.0022) and decreased at high (>0.0073) gelatin wt ratios. Analysis of the effect of gelatin on the emission bandwidth, the stretching exponent beta, and the variation of lifetime across the emission band indicated that matrix dynamic site heterogeneity increased at low and decreased at high gelatin wt ratios. These results provide a novel insight into the complex dynamic effects of the gelatin polymer on the molecular mobility of the amorphous sucrose matrix.     

The effect of salts on molecular mobility in amorphous sucrose monitored by erythrosin B phosphorescence

Salts are present in most amorphous biomaterials such as dried or frozen solid foods, plant seeds, and bacterial spores, and in some pharmaceutical formulations. However, knowledge of how salts modulate the physical properties of amorphous solid sugars, a major component in these systems, is lacking. We have used phosphorescence of the triplet probe erythrosin B (Ery B) to monitor molecular mobility in amorphous sucrose films (dried against P(2)O(5)) containing the salts NaCl, MgCl(2), CaCl(2), NaAcetate, Na(3)Citrate, NaH(2)PO(4), or Na(2)HPO(4) at a mole ratio of 0.2:1 (salt/sucrose). All the salts examined, except NaH(2)PO(4), significantly increased the phosphorescence lifetime of Ery B over the temperature range from 5 to 100 degrees C. This increase is due to a reduction in the rate of collisional quenching of the triplet state due to interactions with the matrix, indicating that these salts decreased the matrix molecular mobility. NaAcetate, Na(3)Citrate, and Na(2)HPO(4) decreased mobility more than NaCl, CaCl(2), or MgCl(2), perhaps due to specific hydrogen bonding interactions between the anion and sucrose. Systematic variations in the probe emission lifetime across the excitation and emission bands at 25 degrees C indicate that there are sites of different mobilities within amorphous solid sucrose; this dynamic site heterogeneity was enhanced in the presence of the divalent cationic salts MgCl(2) and CaCl(2). These results suggest that salts may play a significant role in modulating the mobility, and thus the long-term stability, of amorphous biological matrixes.     

The Effect of Molecular Size on Molecular Mobility in Amorphous Oligosaccharides

The physical properties and especially the molecular mobility of amorphous carbohydrate matrixes directly influence the stability of foods, feeds, and pharmaceuticals and the dessication tolerance of animals and plants during anhydrobiosis. Phosphorescence of the sodium salt of erythrosin B was used to investigate the local molecular mobility in pure amorphous solids of a homologous series of malto-oligosaccharides (maltose, G₂; maltotriose, G₃; maltotetraose, G₄; maltopentaose, G₅; maltohexaose, G₆; and maltoheptaose, G₇); sucrose and maltodextrin DE18 (a hydrolytic fraction of starch) were investigated for comparison. Measurements of the temperature-dependence of the phosphorescence emission energy, an indicator of the extent of local dipolar relaxation, and the phosphorescence emission lifetime, an indicator of the rate of collisional quenching of the excited state by matrix molecules, demonstrate that the local matrix molecular mobility increases with molecular size, and thus, with an increase in T _g, in these glucose oligosaccharides. Master curves of the spectroscopic measures of matrix mobility for each oligosaccharide, plotted against T–T _g, were not superimposable, suggesting that local properties of the amorphous sugar matrixes, rather than T _g per se, influence local matrix mobility. Indicators of spectral heterogeneity also varied with molecular size, indicating that dynamic site heterogeneity also increased with molecular size and thus, T _g. These results emphasize the importance of additional research in developing appropriate “molecular rules” for designing amorphous matrix systems with better long-term stability for foods, feeds, or pharmaceuticals.     

The effect of sodium chloride on molecular mobility in amorphous sucrose detected by phosphorescence from the triplet probe erythrosin B

Phosphorescence from the triplet probe erythrosin B provides spectroscopic characteristics such as emission energy and lifetime that are specifically sensitive to molecular mobility of the local environment. This study used phosphorescence of erythrosin B to investigate how variation in NaCl content modulated the mobility of the amorphous sucrose matrix over the temperature range from 5 to 100 degrees C. Addition of NaCl increased the emission energy and the energy difference with excitation at the absorption maximum and the red edge, and increased the lifetime by reducing the non-radiative decay rate in the glass as well as in the undercooled liquid in a concentration dependent manner, indicating that NaCl decreased the matrix molecular mobility. Emission energy and lifetime increased with increasing NaCl content up to a maximum at NaCl/sucrose mole ratio of approximately 0.5; above 0.5 mole ratio, the effect of NaCl was less significant and appeared to be opposed by increasing plasticization by residual water. Changes in the width of the distribution of the emission energy and lifetime and variation in the lifetime with excitation and emission wavelength indicated that NaCl increased the spectral heterogeneity and thus increased the extent of dynamic site heterogeneity. These results are consistent with a physical model in which sodium and chloride ions interact with sucrose OH by ion-dipole interactions, forming clusters of less mobile molecules within the matrix.     

Molecular mobility and the glass transition in amorphous glucose, maltose, and maltotriose

We have used measurements of the phosphorescence intensity decay of the triplet probe erythrosin B, dispersed in amorphous glucose, maltose, and maltotriose at probe:sugar mole ratios of approximately 1:10(4), to monitor the molecular mobility of the sugar matrix in the glass and melt around the glass-transition temperature (Tg). Intensity decays were well fit using a stretched-exponential decay model in which the Kohlrausch-Williams-Watts lifetime tau and the stretching exponent beta are the physically meaningful parameters. When normalized to the glass-transition temperature, the erythrosin lifetime decreased in the order glucose>maltose>maltotriose. Analysis of the lifetime provided an estimate of the collisional quenching constant for deexcitation of the triplet state (kTS0); kTS0 increased in the order glucosemaltose>maltotriose, indicating that the lifetime heterogeneity increased in the order glucose相似文献   

The Effect of Glycerol on Molecular Mobility in Amorphous Sucrose Detected by Phosphorescence of Erythrosin B

Luminescence from the triplet probe erythrosin B provides spectroscopic characteristics such as emission energy and lifetime that are sensitive to molecular mobility of the local solvent environment. This study investigated how variation in glycerol content influences the properties of an amorphous sucrose matrix by monitoring phosphorescence of erythrosin B over the temperature range from 5 to 100°C. Emission energy, lifetime, and red-edge excitation data revealed that glycerol affected the mobility of amorphous sucrose matrix primarily through plasticization when the mole ratio of glycerol/sucrose was above 0.27, resulting in a decrease in emission energy (ν _p), lifetime (τ) and energy difference (Δν _P) with excitation at the absorption peak and red edge and an increase in the nonradiative, collisional quenching rate k _TS0. At mole ratios ≤0.27 and at temperatures below the matrix T _g, glycerol exhibited an “antiplasticization” effect, as indicated by higher values of emission energy, lifetime, and energy difference and lower values of the matrix collisional quenching rate. Changes in the distribution of emission energy (emission bandwidth) and lifetime, and variation in the emission lifetime vs wavelength showed that glycerol reduced the spectral heterogeneity. These data illustrate the complex effect of a hydrogen bonding solute on the mobility of an amorphous, hydrogen bonded sugar matrix.     

Photophysical Probes of the Amorphous Solid State of Proteins

The properties of amorphous solid proteins influence the texture and stability of low-moisture foods, the shelf-life of pharmaceuticals, and the viability of seeds and spores. We have investigated the relationship between molecular mobility and oxygen permeability in dry food protein films—bovine α-lactalbumin (α-La), bovine β-lactoblobulin (β-Lg), bovine serum albumin (BSA), soy 11S globulin, and porcine gelatin—using phosphorescence from the triplet probe erythrosin B. Measurements of the phosphorescence decay in the absence (nitrogen) and presence (air) of oxygen versus temperature provide estimates of the non-radiative decay rate for matrix-induced quenching (k _TS0) and oxygen quenching (k _Q[O₂]) of the triplet state. Since the oxygen quenching constant is the product of the oxygen solubility ([O₂]) and a term (k _Q) proportional to the oxygen diffusion coefficient, it is a measure of the oxygen permeability through the films. For all proteins except gelatin, Arrhenius plots of k _TS0 reveal a gradual increase of apparent activation energy across a broad temperature range starting at ∼50 °C; this suggests that there is a steady increase in the available modes of molecular motion with increasing temperature within the protein matrix. Arrhenius plots for k _Q[O₂] were linear for all proteins with activation energies ranging from 24 to 29 kJ/mol. The magnitude of the oxygen quenching constants varied in the different proteins; the rates were approximately 10-fold higher in α-La, β-Lg, and BSA than in 11S glycinin and gelatin. Although the rate of oxygen permeability was not directly affected by the increased mobility of the protein matrix, plots of k _Q[O₂] versus k _TS0 were linear over nearly three orders of magnitude in the protein films, suggesting that the matrix mobility plays a specific role in modulating oxygen permeability. This effect may reflect differences in matrix-free volume that directly influence both mobility and oxygen solubility.     

Triplet-state detection of labeled proteins using fluorescence recovery spectroscopy

The experimental procedures for detecting the triplet states of chromophores in solutions (cuvettes) by fluorescence recovery spectroscopy (FRS) are described in detail, together with applications in studies of protein structure and protein-cell interactions in the microsecond to millisecond time domain. The experimental configuration has been characterized by measuring the emission intensities and anisotropies of eosin and erythrosin immobilized in poly(methyl methacrylate). The fluorescence data are compared with those from phosphorescence emission measurements and with theoretical predictions. Triplet-state lifetimes were obtained in 5 mM phosphate buffer, pH 7.0, of concanavalin A labeled with eosin, tetramethylrhodamine, and fluorescein and of alpha 2-macroglobulin labeled with the first two probes. In the case of labeled concanavalin A, iodide quenching measurements gave bimolecular rate constants of approximately 10(9) M-1 s-1. The usefulness of FRS for studying protein-cell interactions is exemplified with eosin-labeled concanavalin A bound to living A-431 human epidermoid carcinoma cells. Finally, the advantages and disadvantages of the technique are compared to those of the alternative phosphorescence emission method.     

An optical method for measurement of dioxygen concentration based upon quenching of phosphorescence

An optical method for measuring oxygen concentrations in aqueous solutions is described. This method is based upon the oxygen-dependent quenching of phosphorescence. Phosphorescence excitation and emission spectra and lifetimes of some of the probe molecules suitable for measurement of oxygen in aqueous solutions are given. The probes include fluorescein derivatives, 4'5'-diiodofluorescein, eosin Y, 5(and 6)-carboxyeosin, erythrosin, and 5(and 6)-carboxyerythrosin as well as the Zn(II), Y(III), Sn(IV), Lu(III), and Pd(II) derivatives of meso-tetra-(4-sulfonatophenyl)-porphine, meso-tetra-(N-methyl-4-pyridyl)-porphine and coproporphyrin. The phosphorescence lifetimes of the given probes were found to depend upon the oxygen concentration by a simple Stern-Volmer relationship with a quenching constant of approximately 10(9) M-1 S-1. Binding of the molecules to bovine serum albumin decreased the quenching constant for oxygen by approximately an order of magnitude and also inhibited probe self-quenching, indicating that at the protein binding site the probes are somewhat protected from collision with quenchers. The use of this optical method for measuring oxygen is demonstrated for reactions catalyzed by glucose oxidase and by cytochrome c oxidase. It is shown that, using this method oxygen concentrations can be measured from approximately 250 microM (air saturation) down to the nanomolar range.     

Monitoring membrane protein rotational diffusion using time-averaged phosphorescence

Rotational motions of membrane proteins have previously been measured using time-dependent phosphorescence techniques. This paper discusses a method of examining membrane protein mobility at temperatures relevant to biological systems, using a technique similar to steady-state fluorescence. The method is demonstrated using sarcoplasmic reticulum ATPase labelled with erythrosin isothiocyanate, both in its natural condition and crosslinked by incubation with glutaraldehyde. The experimentally-observed dependence of phosphorescence anisotropy on temperature is compared to a calculated anisotropy-temperature curve. Comparison is made between the anisotropy decay curves obtained by time-averaged phosphorescence and steady-state fluorescence.     

Characterization of lens alpha-crystallin tryptophan microenvironments by room temperature phosphorescence spectroscopy

Room temperature phosphorescence techniques were used to study the structural and dynamic features of the tryptophan residues in bovine alpha-crystallin. Upon excitation at 290 nm, the characteristic signature of tryptophan phosphorescence was observed with an emission maximum at 442 +/- 2 nm. The phosphorescence intensity decay was biphasic with lifetimes of 5.4 ms (71%) and 42 ms (29%). Phosphorescence quenching measurements strongly suggest that each component corresponds to one class of tryptophans with the more buried residues having the longer emission lifetime. Three small-molecule quenchers were surveyed, and in order of increasing quenching efficiency: iodide less than nitrite less than acrylamide. A heavy-atom effect was observed in iodide solutions, and an upper limit of 5% was placed on the quantum yield of triplet formation in iodide-free solutions, while the phosphorescence quantum yield was estimated to be approximately 3.2 x 10(-4). The temperature dependence of the phosphorescence lifetime was measured between 5 and 40 degrees C. Arrhenius plots exhibited discontinuities at 26 and 29 degrees C for the short- and long-lived components, respectively, corresponding to abrupt transitions in segmental flexibility. Denaturation studies revealed conformational transitions between 1 and 2 M guanidine hydrochloride, and 4 and 6 M urea. Long-lived phosphorescence lifetimes of 3 and 7 ms were measured in 6 M guanidine hydrochloride and 8 M urea, respectively, suggesting that some structural features are preserved even at very high concentrations of denaturant. Our studies demonstrate the sensitivity of room temperature phosphorescence spectroscopy to the structure of alpha-crystallin, and the applicability of this technique for monitoring conformational changes in lens crystallin proteins.(ABSTRACT TRUNCATED AT 250 WORDS)     

Tyrosine quenching of tryptophan phosphorescence in glyceraldehyde-3-phosphate dehydrogenase from Bacillus stearothermophilus.

Tyrosine is known to quench the phosphorescence of free tryptophan derivatives in solution, but the interaction between tryptophan residues in proteins and neighboring tyrosine side chains has not yet been demonstrated. This report examines the potential role of Y283 in quenching the phosphorescence emission of W310 of glyceraldehyde-3-phosphate dehydrogenase from Bacillus stearothermophilus by comparing the phosphorescence characteristics of the wild-type enzyme to that of appositely designed mutants in which either the second tryptophan residue, W84, is replaced with phenylalanine or Y283 is replaced by valine. Phosphorescence spectra and lifetimes in polyol/buffer low-temperature glasses demonstrate that W310, in both wild-type and W84F (Trp84-->Phe) mutant proteins, is already quenched in viscous low-temperature solutions, before the onset of major structural fluctuations in the macromolecule, an anomalous quenching that is abolished with the mutation Y283V (Tyr283-->Val). In buffer at ambient temperature, the effect of replacing Y283 with valine on the phosphorescence of W310 is to lengthen its lifetime from 50 micros to 2.5 ms, a 50-fold enhancement that again emphasizes how W310 emission is dominated by the local interaction with Y283. Tyr quenching of W310 exhibits a strong temperature dependence, with a rate constant kq = 0.1 s(-1) at 140 K and 2 x 10(4) s(-1) at 293 K. Comparison between thermal quenching profiles of the W84F mutant in solution and in the dry state, where protein flexibility is drastically reduced, shows that the activation energy of the quenching reaction is rather small, Ea < or = 0.17 kcal mol(-1), and that, on the contrary, structural fluctuations play an important role on the effectiveness of Tyr quenching. Various putative quenching mechanisms are examined, and the conclusion, based on the present results as well as on the phosphorescence characteristics of other protein systems, is that Tyr quenching occurs through the formation of an excited-state triplet exciplex.     

Characterization of tryptophan phosphorescence of aspartate aminotransferase from Escherichia coli.

The Trp phosphorescence spectrum, intensity and decay kinetics of apo-aspartate aminotransferase, pyridoxamine-5P-aspartate-aminotransferase and pyridoxal-5P-aspartate aminotransferase were measured over a temperature range 160-273 K. The fine structure of the phosphorescence spectra in low-temperature glasses, with 0-0 vibrational bands centered at 408, 415 and 417 nm, for both apoenzyme and pyridoxamine-5P-enzyme reveals a marked heterogeneity of the chromophore environments. Only for the pyridoxal-5P form of the enzyme is the triplet emission strongly quenched and, in this case, the spectrum displays a unique 0-0 vibrational band centered at 415 nm. Concomitant to quenching, there is Trp-sensitized delayed fluorescence of the Schiff base, an indication that quenching of the excited triplet state is due, at least in part, to a process of triplet singlet energy transfer to the ketoenamine tautomer. All three forms of the enzyme are phosphorescent for temperatures up to 273 K. However, across the glass transition temperature the pyridoxal-5P enzyme shows a decrease in lifetime-normalized phosphorescence intensity, a thermal quenching that reduces even further the number of phosphorescing residues at ambient temperature. In fluid solution, the triplet decay is nonexponential and multiple lifetimes stress the heterogeneity in dynamical structure of the chromophores' sites. For the pyridoxal-5P enzyme, where only one or at most two residues are phosphorescent at 273 K, the nonexponential nature of the decay implies the presence of different conformers of the protein not interconverting in the millisecond time scale.     

Comparative Phosphorescence Quenching of DNA's of Different Composition

Small amounts of paramagnetic cations quench the phosphorescence of DNA. Although the emission intensity is monotonic with increasing thymine content, the quenching efficiency is not. The cations quench from phosphate sites.     

Time resolved fluorescence and phosphorescence properties of the individual tryptophan residues of barnase: evidence for protein-protein interactions.

Steady-state and time-resolved fluorescence, as well as phosphorescence measurements, were used to resolve the luminescence properties of the three individual tryptophan residues of barnase. Assignment of the fluorescence properties was performed using single-tryptophan-containing mutants and the results were compared with the information available from the study of wild-type and two-tryptophan-containing mutants (Willaert, Lowenthal, Sancho, Froeyen, Fersht, Engelborghs, Biochemistry 1992;31:711-716). The fluorescence and the phosphorescence emission of wild-type barnase is dominated by Trp35, although Trp71 has the strongest intrinsic fluorescence when present alone. Fluorescence emission of these two tryptophan residues is blue-shifted and pH-independent. The fluorescence decay parameters of Trp94 are pH-dependent, and an intramolecular collision frequency of 2 to 5 x 10(9) s(-1) between Trp94 and His18 is calculated. Fluorescence emission of Trp94 is red-shifted. Fluorescence anisotropy decay reveals the local mobility of the individual tryptophan residues and this result correlates well with their phosphorescence properties. Trp35 and Trp71 display a single phosphorescence lifetime, which reflects the rigidity of their environment. Surface Trp94 does not exhibit detectable phosphorescence emission. The existence of energy transfer between Trp71 and Trp94, as previously detected by fluorescence measurements, is also observed in the phosphorescence emission of barnase. Dynamic quenching causes the phosphorescence intensity to be protein-concentration dependent. In addition, fluorescence anisotropy shows concentration dependency, and this can be described by the formation of trimers in solution.     

Effects of cavity-forming mutations on the internal dynamics of azurin

The effects of two single-point cavity-forming mutations, F110S and I7S, on the internal dynamics of azurin from Pseudomonas aeruginosa were probed by the phosphorescence emission of Trp-48, deeply buried in the compact hydrophobic core of the macromolecule. Changes in flexibility of the protein matrix around the chromophore were monitored by the intrinsic phosphorescence lifetime (tau(0)) whereas more general effects on structural fluctuations were deduced from the phosphorescence acrylamide quenching rate constant (k(q)), which measures the diffusion of the solute through the protein fold. The results show a spectacular, 4-5 orders of magnitude, increase of k(q) emphasizing that large amplitude structural fluctuations permitting acrylamide migration to the protein core have been drastically enhanced in each azurin mutant. The large, 12-15 kcal/mol, decrease in the activation enthalpy associated to k(q) suggests that the rate enhancement is caused, rather than through a generalized increase of protein flexibility, by the elimination of an inner barrier to the diffusion process. According to tau(0) the chromophore environment is more fluid with I7S but strikingly more rigid with F110S, demonstrating that when internal cavities are formed local effects on the mobility at the mutation site are unpredictable. Both tau(0) and k(q) reveal a structure tightening role of bound Cd(2+) that correlates with the increase in stability from apo- to holo-azurin. While these alterations in internal dynamics of azurin do not seem to play a role on electron transfer through the central region, the enhanced migration of acrylamide emphasizes that cavities may be critical for the rapid diffusion of substrates to buried, solvent inaccessible sites of enzymes.     

Interaction between cytochrome c and cytochrome c peroxidase: excited-state reactions of zinc- and tin-substituted derivatives

The effect of cytochrome c peroxidase (CCP) and apoCCP on the fluorescence and phosphorescence of Zn and Sn cytochrome c (cyt c) and the effect of cyt c on the fluorescence and phosphorescence of Zn CCP were examined. We found the following: The fluorescence yields of Zn and Sn cyt c were quenched by about 20% by CCP, consistent with energy transfer between the two chromophores with a separation of about 1.8 nm. The phosphorescence spectrum of Zn cyt c (but not Sn cyt c) shifts by 20 nm to the blue upon complexation with either CCP or apoCCP; at the same time the phosphorescence lifetime of Zn cyt c decreases from 12 +/- 2 to 6 ms with apoCCP addition. Zn CCP phosphorescence decay increases from 8.3 to 9.1 ms upon addition of poly(L-lysine) used to mimic cyt c. It is concluded from these results that binding of the redox partner or an analogue to Zn CCP and Zn cyt c results in a conformational change. The respective phosphorescence lifetimes of Zn and Sn cyt c were 13 and 3 ms in the absence of CCP and 1.6 and 1.1 ms in the presence of CCP; this corresponds to a quenching rate due to CCP of 519 and 570 s-1, for Zn and Sn cyt c, respectively. The phosphorescence of Zn CCP is also affected by native cyt c but is dramatically less than the complementary pair; the quenching rate constant is 17 s-1.(ABSTRACT TRUNCATED AT 250 WORDS)