Fluorescence quenching of the buried tryptophan residue of cod parvalbumin

Cod parvalbumin (isotype III) is a single tryptophan-containing protein. The fluorescence characteristics of this tryptophan residue (lambda em approximately 315 nm) suggest that it is buried from solvent and that it is located in an apolar core of the protein. Solute quenching studies of the tryptophan fluorescence of parvalbumin reveal dynamic quenching rate constants, kq, of 1.1 X 10(8) and 2.3 X 10(9) M-1 s-1 (at 25 degrees C) with acrylamide and oxygen, respectively, as quenchers. From temperature dependence studies, activation energies of 6.5 +/- 1.5 and 6.0 +/- 0.5 kcal/mol are found for acrylamide and oxygen quenching. The kq for acrylamide quenching is found to be relatively unchanged (+/- 10%) by an 8-fold increase in the bulk viscosity (glycerol/water mixture). These temperature and viscosity studies argue that the acrylamide quenching process involves a dynamic penetration of the quencher, facilitated by fluctuations in the protein's structure.     

Effect of alkaline PH on sunflower 11S Protein

The effect of alkaline PH on sunflower 1 1S Protein has been monitored by the techniques of ultracentrifugation, Polyacrylamide gel electroPhoresis, turbidity, viscosity, ultraviolet absorPtion sPectra and fluorescence sPectra. Both ultracentrifugation and Polyacrylamide gel electroPhoresis show the dissociation of the Protein with increase in PH. Turbidity values decrease with PH while viscosity increases. With increase in PH absorbance of the Protein solution increases and there is a red shift in the absorPtion maximum. Fluorescence quenching and a red shift in the emission maximum are also observed. Both dissociation and denaturation of the Protein occur. Analysis of turbidity, viscosity and fluorescence data suggests that aPParently denaturation follows dissociation.     

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.     

Micronomicin/tobramycin binding with DNA: fluorescence studies using of ethidium bromide as a probe and molecular docking analysis

Two aminoglycosides, micronomicin (MN), and tobramycin (TB), binding with DNA were studied using various spectroscopic techniques including fluorescence, UV–Vis, FT-IR, and CD spectroscopy coupled with relative viscosity and molecular docking. Studies of fluorescence quenching and time-resolved fluorescence spectroscopy all revealed that MN/TB quenching the fluorescence of DNA–EB belonged to static quenching. The binding constants and binding sites were obtained. The values of ΔH, ΔS, and ΔG suggested that van der Waals force or hydrogen bond might be the main binding force. FT-IR and CD spectroscopy revealed that the binding of MN/TB with DNA had an effect on the secondary structure of DNA. Binding mode of MN/TB with DNA was groove binding which was ascertained by viscosity measurements, CD spectroscopy, ionic strength, melting temperature (T_m), contrast experiments with single stranded (ssDNA), and double stranded DNA (dsDNA). Molecular docking analysis further confirmed that the groove binding was more acceptable result.     

Effect of sodium dodecyl sulphate on the high molecular weight protein fraction of mustard (Brassica juncea) and rapeseed (Brassica campestris)

The effect of sodium dodecyl sulphate on mustard and rapeseed 12S protein has been monitored by the techniques of ultracentrifugation, viscosity, difference spectra and fluorescence spectrophotometry. At low concentration of sodium dodecyl sulphate (<3.47 mM) mustard protein undergoes aggregation and at higher concentrations it dissociates to 1.8 S protein, the dissociation being complete at 17.3 mM sodium dodecyl sulphate. The rapeseed protein, on the other hand, undergoes dissociation at all the concentrations of sodium dodecyl sulphate. The reduced viscosity values of mustard protein in the presence of the denaturant are higher than those of rapeseed protein. Similarly in difference spectra change in absorbance values of mustard protein are higher.’ The relative fluorescence intensity of the mustard protein increases with sodium dodecyl sulphate concentration, upto 0.87 mM and this is followed by fluorescence quneching at higher denaturant concentrations. However, with the rapeseed protein fluorescence quenching was observed at all concentrations of sodium dodecyl sulphate.     

Dielectric relaxation in a single tryptophan protein.

Although dielectric relaxation can significantly affect the intrinsic fluorescence properties of a protein, usually it is fast compared to fluorescence timescales and needs to be slowed down by adding viscogens or lowering temperature before its impact on fluorescence can be studied. We report here a remarkable blue shift in fluorescence upon bimolecular quenching in the single-tryptophan thermostable protein Bj2S, the 2S seed albumin from Brassica juncea, at ambient temperature and viscosity. The magnitude of the blue shift ( approximately 5 nm at 50% quenching by acrylamide) is striking in a single-tryptophan protein and is attributed to a slowly relaxing dielectric environment in Bj2S from red edge excitation, steady-state polarization and time-resolved fluorescence experiments. Our results have important implications on interpretation of fluorescence of proteins with highly constrained backbones and in designing model systems for studying slow protein solvation dynamics using Trp fluorescence as the reporter probe.     

Fluorescence quenching of methyl-2-aminobenzoate in the presence of beta-cyclodextrin: A model for the dynamic quenching of chromophores in hydrophobic regions of biopolymers

The binding constant of methyl-2-aminobenzoate to beta-cyclodextrin was determined by fluorescence titration to be 92.1M^?1 at 25°C in pH 7 buffer. Beta-cyclodextrin dramatically protects methyl-2-aminobenzoate against quenching by iodate and protects, though much less efficiently, against the smaller quencher, iodide. The observed decrease in fluorescence lifetime of the methyl-2-aminobenzoate-beta-cyclodextrin complex on addition of quencher indicates that the quenching mechanism is collisional (dynamic). The dependence of quenching rate on solvent viscosity is less than expected from simple theoretical considerations. However, the extent of beta-cyclodextrin protection is essentially viscosity-independent. These model studies show the usefulness of iodate as a quencher and encourage further attempts at quantitative interpretation of quenching studies on chromophores attached to biopolymers.     

Gated quenching of intrinsic fluorescence and phosphorescence of globular proteins. An extended model.

We present a theoretical model to account for the quenching data of macromolecular fluorescence and phosphorescence when the accessibility to the quencher is gated by a dynamic mechanism coupled to the fluctuation of the macromolecular matrix. We show that the model currently in use to interpret gated quenching processes gives only approximate results in both qualitative and quantitative terms, and it can be regarded as a specific case of the presented model. We show that the gating dynamics affect both the apparent accessibility (alpha obs) and Ksv values obtained by the modified Stern-Volmer plot. The effect of gating on alpha obs and Ksv depends upon the relative rate of gating compared to the excited state lifetime. The model allows us to predict the effect of viscosity on quenching if it takes place by a gated mechanism. The prediction can and is, in this case, compared to the existing data on glycerol effects on acrylamide quenching of the tryptophan fluorescence in RNAse T1. The result shows that a simple gated model is not compatible with the observed quenching behavior.     

Diffusion of small molecules through the structure of myoglobin. Environmental effects

The effect of the ambient solvent viscosity on the mobility of small molecules within myoglobin was studied by substituting Zn-protoporphyrin (ZnPP) for the native Fe-protoporphyrin and using it as an optical probe in the protein (ZnPPMb). The quenching of the ZnPPMb triplet state by oxygen, by anthraquinonesulfonate, and by methyl viologen was followed by exciting it with a laser flash and measuring its decay rate as a function of quencher concentration. The quenching rate constants were taken to measure the diffusion rate of the quencher within the protein. At room temperature, these constants were determined in aqueous and in 37% and 55% (by weight) glycerol-water solutions by measuring the ZnPPMb-delayed fluorescence at 606 nm. It was found that although the quenching rate constants varied the activation energies in the protein were very similar for the different quenchers. In aqueous solution, Ea = 6.0-7.4 kcal/mol; in 37% glycerol, Ea = 6.8-7.5 kcal/mol; and in 55% glycerol, Ea = 8.5-9.2 kcal/mol. The quenching rate of ZnPPMb by oxygen was also measured between 190K and 293K in 80% glycerol, and its triplet decay in the absence of oxygen was determined down to 120K in 88% glycerol. In all experiments, the quenching rates in the protein were compared to those of Zn-hematoporphyrin in the same solvent. The results are discussed in terms of Northrup and McCammon's gated reaction theory.(ABSTRACT TRUNCATED AT 250 WORDS)     

Oxygen distribution and migration within Mbdes Fe and Hbdes Fe. Multifrequency phase and modulation fluorometry study.

Quenching of the intensity and lifetime of porphyrin fluorescence from Mbdes Fe and Hbdes Fe (iron-free myoglobin and hemoglobin) by oxygen was investigated using a multifrequency cross-correlation phase fluorometer. The single exponential decay characteristic of porphyrin emission of Mbdes Fe and Hbdes Fe became doubly exponential upon application of oxygen pressure. The results were interpreted in terms of a general model of dynamic quenching of fluorescence in globular proteins. The model accounted for the rate k+ of acquisition of quencher by the protein, the exit rate k- of quencher from the protein, and the migration rate chi of quencher in the protein interior. The values of k+, k-, and chi were different for Mbdes Fe and Hbdes Fe. The addition of 40% sucrose, which increased the bulk viscosity sixfold, modified these rates. These results are discussed and compared with previous quenching studies on proteins. The significance of these results and the model for the interpretation of protein quenching studies is emphasized.     

Viscosity dependence of the solute quenching of the tryptophanyl fluorescence of proteins

We have studied the viscosity dependence of the acrylamide quenching of the fluorescence on the internal tryptophan residues in cod parvalbumin and ribonuclease T1, as well as the model systems. N-acetyl-L-tryptophanamide and glucagon. For the latter systems, the apparent rate constant, kq(app), for acrylamide quenching shows a typical diffusion-limited behavior. For parvalbumin and ribonuclease T1, however, the viscosity dependence of kq(app) is quite different. There is little change in the kq(app) values on increasing the bulk viscosity from 1 to 10 cP (by addition of glycerol), but a further increase from 10 to 100 cP results in a significant reduction in the kq(app). Both an unfolding mechanism and a quencher penetration mechanism are considered to explain the results. Only the penetration mechanism is found to be consistent, and our data are interpreted as indicating that the rate-limiting step for quenching goes from being that of diffusion through the protein matrix, at low viscosity, to diffusion through the bulk solvent, at high viscosity. By also considering the Kramers' relationship in fitting our data, we are able to obtain insight regarding the coupling between internal fluctuations in the structure of the protein and motion of the bulk solvent. For parvalbumin and ribonuclease T1, the internal dynamics are found to be very weakly coupled to the bulk.     

Some aspects of studies of thermal transitions in proteins by means of their intrinsic fluorescence

The changes in intrinsic fluorescence parameters induced by thermal transitions in proteins are developed on the background of the common thermal fluorescence quenching due to an activation of collisions between the excited chromophores and neighbouring quenching groups. Two methods of separation of the thermai quenching and conformational change contributions to the temperature dependence of the fluorescence parameters are presented. One is based on the use of the linearity of the plots of the reciprocal fluorescence quantum yield, l/q, vs. the t/η ratio (T. temperature; η, solvent viscosity) for native proteins containing a single fluorescing chromophore (T.L. Bushueva, E.P. Busel and E.A. Burstein, Biochim. Biophys. Acta 534 (1978) 141). The other method is based on a consideration of the phase plots for the tryptophan fluorescence of proteins (fluorescence intensity at a fixed wavelength vs. intensity at any other fixed wavelength). The methods have been used for a study of the thermal transitions in Mg²⁺-loaded whiting parvalbumin (tryptophan fluorescence), Mg²⁺-loaded pike parvalbumins pI 4.2 (tyrosine fluorescence) and pI 5.0 (phenylalanine fluorescence), and Ca²⁺-loaded bovine α-lactalbumin (tryptophan fluorescence). The thermal denaturation curves for the parvalbumins show two-stepped character. The main change of the protein conformation occurs at the higher temperature step. Comparison of the fluorescence data with the microcalorimetry results shows that the maxima of the asymmetric heat sorption peaks for pike parvalbumins correlate with the mid-points of the higher temperature steps of the fluorimetric curves.     

A quantitative determination of photochemical and non-photochemical quenching during the slow phase of the chlorophyll fluorescence induction curve of bean leaves

Estimations of the changes in the reduction-oxidation state of Photosystem II electron acceptors in Phaseolus vulgaris leaves were made during the slow decline in chlorophyll fluorescence emission from the maximal level at P to the steady-state level at T. The relative contributions of photochemical and non-photochemical processes to the fluorescence quenching were determined from these data. At a low photon flux density of 100 μmol · m^?2 · s^?1, non-photochemical quenching was the major contributor to the fluorescence decline from P to T, although large charges were observed in photochemical quenching immediately after P. On increasing the light intensity 10-fold, the contribution of photochemical processes to fluorescence quenching was markedly diminished, with nearly all the P-to-T fluorescence decline being attributable to changes in non-photochemical quenching. The possible factors responsible for changes in non-photochemical quenching within the leaves are discussed.     

Photoprotection in the lichen Parmelia sulcata: the origins of desiccation-induced fluorescence quenching

Lichens, a symbiotic relationship between a fungus (mycobiont) and a photosynthetic green algae or cyanobacteria (photobiont), belong to an elite group of survivalist organisms termed resurrection species. When lichens are desiccated, they are photosynthetically inactive, but upon rehydration they can perform photosynthesis within seconds. Desiccation is correlated with both a loss of variable chlorophyll a fluorescence and a decrease in overall fluorescence yield. The fluorescence quenching likely reflects photoprotection mechanisms that may be based on desiccation-induced changes in lichen structure that limit light exposure to the photobiont (sunshade effect) and/or active quenching of excitation energy absorbed by the photosynthetic apparatus. To separate and quantify these possible mechanisms, we have investigated the origins of fluorescence quenching in desiccated lichens with steady-state, low temperature, and time-resolved chlorophyll fluorescence spectroscopy. We found the most dramatic target of quenching to be photosystem II (PSII), which produces negligible levels of fluorescence in desiccated lichens. We show that fluorescence decay in desiccated lichens was dominated by a short lifetime, long-wavelength component energetically coupled to PSII. Remaining fluorescence was primarily from PSI and although diminished in amplitude, PSI decay kinetics were unaffected by desiccation. The long-wavelength-quenching species was responsible for most (about 80%) of the fluorescence quenching observed in desiccated lichens; the rest of the quenching was attributed to the sunshade effect induced by structural changes in the lichen thallus.     

Detection of energy transfer between tryptophan residues in the tubulin molecule and bound bis(8-anilinonaphthalene-1-sulfonate), an inhibitor of microtubule assembly, that binds to a flexible region on tubulin

The fluorescent apolar probe bis(8-anilinonaphthalene-1-sulfonate) (Bis-ANS) is a potent inhibitor of microtubule assembly that binds to tubulin at a hitherto uncharacterized site distinct from those of the antimitotic drugs. We have found that energy transfer between tryptophan residues and bound Bis-ANS leads to quenching of the intrinsic tubulin fluorescence. The quenching is biphasic, implying two types of Bis-ANS binding sites. The estimated Kd values are 2.7 and 22.2 microM, consistent with reported values for the primary and secondary Bis-ANS binding sites. Preincubation of tubulin at 37 degrees C results in increased quenching of tryptophan fluorescence without any effect on the Kd values, suggesting localized structural change in the protein around the Bis-ANS binding sites. Concentration-dependent depolarization of Bis-ANS fluorescence was observed, suggesting energy transfer among bound Bis-ANS molecules. Such a concentration-dependent decrease in fluorescence polarization was not observed with 8-anilinonaphthalene-1-sulfonate (1,8-ANS), the monomeric form of Bis-ANS. Perrin-Weber plots were obtained for bound Bis-ANS and 1,8-ANS by varying the viscosity with sucrose. The rotational relaxation times calculated for Bis-ANS and 1,8-ANS are 18 and 96 ns, respectively. Comparison with the theoretical value (125 ns) suggests that Bis-ANS binds to a flexible region of tubulin. This, coupled with the fact that Bis-ANS, but not 1,8-ANS, inhibits microtubule assembly, suggests that the region in the tubulin molecule responsible for microtubule assembly is relatively flexible.     

Protein fluorescence quenching by small molecules: protein penetration versus solvent exposure

Experiments were done to test the thesis that acrylamide and similar small molecules can penetrate into proteins on a nanosecond time scale. The approach taken was to measure the pattern of fluorescence quenching exhibited by quenching molecules differing in molecular character (size, polarity, charge) when these are directed against protein tryptophans that cover the whole range of tryptophan accessibility. If quenching involves protein penetration and internal quencher migration, one expects that larger quenchers and more polar quenchers should display lesser quenching. In fact, no significant dependence on quencher character was found. For proteins that display measurable quenching, the disparate quenchers studied display very similar quenching rate constants when directed against any particular protein tryptophan. For several proteins having tryptophans known to be buried, no quenching occurs. These results are not consistent with the view that the kinds of small molecules studied can quite generally penetrate into and diffuse about within proteins at near-diffusion-limited rates. Rather the results suggest that when quenching is observed, the pathway involves encounters with tryptophans that are partially exposed at the protein surface. Available crystallographic results support this conclusion.     

Analysis of fluorescence quenching of ribosome-bound virginiamycin S

The two virginiamycin components VM and VS interact synergistically with bacterial ribosomes in vitro and in vivo. Ribosome affinity for virginiamycin S increases about 10-fold upon incubation with virginiamycin M. This effect has been previously traced by spectrofluorimetric measurement based on the enhancement of virginiamycin S fluorescence upon its binding to the 50 S ribosomal subunit. In the present work the action of two virginiamycin S fluorescence quenchers, acrylamide and iodide, has been explored to gather information about the accessibility of ribosome-bound virginiamycin S and the variation of the accessibility level in the presence of virginiamycin M. Both acrylamide (non-ionized quencher) and iodide (ionized quencher) proved powerful quenchers of free virginiamycin S solutions. Since a comparable effect was obtained on 3- hydroxypicolinamide , the latter was indicated as the part of the molecule involved in the fluorescence effect. Fluorescence quenching by either agent was of the dynamic, i.e. collisional, type. Such an inference was based on the fact that these quenchers merely modified the emission spectrum (not the absorption spectrum), the bimolecular rate constant for the quenching process decreased linearly with the viscosity of the medium (static-type quenching is viscosity-independent), and that linear Stern-Volmer plots were obtained. The quenching ability of both agents underwent a sharp decrease in the presence of ribosomes; however, the Stern-Volmer equation was followed only in the case of acrylamide, whereas Lehrer 's relationship had to be applied in the case of iodide. When ribosomes were incubated with virginiamycin M, the fluorescence quenching ability of acrylamide and iodide was significantly reduced. Conclusions are as follows: a) the 3- hydroxypicolinyl residue of virginiamycin S is buried within an open well on the ribosome surface and is likely to be involved in the interaction with the binding site; b) the accessibility to the well is partly controlled by electrostatic forces; c) interaction of ribosomes with virginiamycin M entails a conformational change whereby the access to the well is reduced. These findings provide a molecular explanation for the previously observed increase of the association constant of virginiamycin S to ribosomes incubated with virginiamycin M which was found to be due to the decrease of the dissociation rate constant (the association rate constant remains practically the same).     

Tryptophan quenching as linear sensor for oxygen binding of arthropod hemocyanins

Oxygen binding of hemocyanins results in an absorption band around 340nm and a strong quenching of the intrinsic tryptophan fluorescence. Our study analyses in detail the fluorescence quenching within two hemocyanins, a hexamer (Panulirus interruptus) and a 4 x 6-mer (Eurypelma californicum). Based on the comparison of calculated and measured transfer efficiencies we could show that: (1) For both hemocyanins FRET (fluorescence resonance energy transfer) is exclusively responsible for quenching of the tryptophan fluorescence upon oxygen binding. (2) Tryptophan quenching by FRET is independent of the oxy- or deoxy conformation of the protein. (3) The quenching takes place at the subunit level only and the oligomerization of both hemocyanins has no influence on the amount of quenching. Therefore, tryptophan fluorescence is a linear sensor for bound oxygen. It can be used as a model-free signal to investigate oxygen binding of hemocyanins at all aggregation levels. Furthermore it may provide a new way to analyse oxygen binding of phenoloxidases.     

DNA-binding and cleavage studies of novel copper(II) complex with L-phenylalaninate and 1,4,8,9-tetra-aza-triphenylene ligands

DNA-binding properties of novel copper(II) complex [Cu(l-Phe)(TATP)(H(2)O)](+), where L-Phe=L-phenylalaninate and TATP=1,4,8,9-tetra-aza-triphenylene are investigated using electronic absorption spectroscopy, fluorescence spectroscopy, voltammetry and viscosity measurement. It is found that the presence of calf thymus DNA results in a hypochromism and red shift in the electronic absorption, a quenching effect on fluorescence nature of ethidium bromide-DNA system, an enhanced response on voltammograms of [Co(phen)(3)](3+/2+)-DNA system, and an obvious change in viscosity of DNA. From absorption titration, fluorescence analysis and voltammetric measurement, the binding constant of the complex with DNA is calculated. The latter two methods reveal the stronger binding of [Cu(l-Phe)(TATP)(H(2)O)](+) complex to double strand DNA by the moderate intercalation than [Co(phen)(3)](3+). Such a binding induces the cleavage of plasmid pBR322 DNA in the presence of H(2)O(2).     

The causes of altered chlorophyll fluorescence quenching induction in the Arabidopsis mutant lacking all minor antenna complexes

Non-photochemical quenching (NPQ) of chlorophyll fluorescence is the process by which excess light energy is harmlessly dissipated within the photosynthetic membrane. The fastest component of NPQ, known as energy-dependent quenching (qE), occurs within minutes, but the site and mechanism of qE remain of great debate. Here, the chlorophyll fluorescence of Arabidopsis thaliana wild type (WT) plants was compared to mutants lacking all minor antenna complexes (NoM). Upon illumination, NoM exhibits altered chlorophyll fluorescence quenching induction (i.e. from the dark-adapted state) characterised by three different stages: (i) a fast quenching component, (ii) transient fluorescence recovery and (iii) a second quenching component. The initial fast quenching component originates in light harvesting complex II (LHCII) trimers and is dependent upon PsbS and the formation of a proton gradient across the thylakoid membrane (ΔpH). Transient fluorescence recovery is likely to occur in both WT and NoM plants, but it cannot be overcome in NoM due to impaired ΔpH formation and a reduced zeaxanthin synthesis rate. Moreover, an enhanced fluorescence emission peak at ~679?nm in NoM plants indicates detachment of LHCII trimers from the bulk antenna system, which could also contribute to the transient fluorescence recovery. Finally, the second quenching component is triggered by both ΔpH and PsbS and enhanced by zeaxanthin synthesis. This study indicates that minor antenna complexes are not essential for qE, but reveals their importance in electron stransport, ΔpH formation and zeaxanthin synthesis.