Phycobilin/chlorophyll excitation equilibration upon carotenoid-induced non-photochemical fluorescence quenching in phycobilisomes of the cyanobacterium Synechocystis sp. PCC 6803

To determine the mechanism of carotenoid-sensitized non-photochemical quenching in cyanobacteria, the kinetics of blue-light-induced quenching and fluorescence spectra were studied in the wild type and mutants of Synechocystis sp. PCC 6803 grown with or without iron. The blue-light-induced quenching was observed in the wild type as well as in mutants lacking PS II or IsiA confirming that neither IsiA nor PS II is required for carotenoid-triggered fluorescence quenching. Both fluorescence at 660 nm (originating from phycobilisomes) and at 681 nm (which, upon 440 nm excitation originates mostly from chlorophyll) was quenched. However, no blue-light-induced changes in the fluorescence yield were observed in the apcE(-) mutant that lacks phycobilisome attachment. The results are interpreted to indicate that interaction of the Slr1963-associated carotenoid with--presumably--allophycocyanin in the phycobilisome core is responsible for non-photochemical energy quenching, and that excitations on chlorophyll in the thylakoid equilibrate sufficiently with excitations on allophycocyanin in wild type to contribute to quenching of chlorophyll fluorescence.     

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.     

Phycobilin/chlorophyll excitation equilibration upon carotenoid-induced non-photochemical fluorescence quenching in phycobilisomes of the cyanobacterium Synechocystis sp. PCC 6803

To determine the mechanism of carotenoid-sensitized non-photochemical quenching in cyanobacteria, the kinetics of blue-light-induced quenching and fluorescence spectra were studied in the wild type and mutants of Synechocystis sp. PCC 6803 grown with or without iron. The blue-light-induced quenching was observed in the wild type as well as in mutants lacking PS II or IsiA confirming that neither IsiA nor PS II is required for carotenoid-triggered fluorescence quenching. Both fluorescence at 660 nm (originating from phycobilisomes) and at 681 nm (which, upon 440 nm excitation originates mostly from chlorophyll) was quenched. However, no blue-light-induced changes in the fluorescence yield were observed in the apcE⁻ mutant that lacks phycobilisome attachment. The results are interpreted to indicate that interaction of the Slr1963-associated carotenoid with - presumably - allophycocyanin in the phycobilisome core is responsible for non-photochemical energy quenching, and that excitations on chlorophyll in the thylakoid equilibrate sufficiently with excitations on allophycocyanin in wild type to contribute to quenching of chlorophyll fluorescence.     

Characterisation of the effects of Antimycin A upon high energy state quenching of chlorophyll fluorescence (qE) in spinach and pea chloroplasts

High energy state quenching of chlorophyll fluorescence (qE) is inhibited by low concentrations of the inhibitor antimycin A in intact and osmotically shocked chloroplasts isolated from spinach and pea plants. This inhibition is independent of any effect upon pH (as measured by 9-aminoacridine fluorescence quenching). A dual control of qE formation, by pH and the redox state of an unidentified chloroplast component, is implied. Results are discussed in terms of a role for qE in the dissipation of excess excitation energy within photosystem II.Abbreviations 9-AA_max = Maximum yield of 9-aminoacridine fluorescence - DCMU = 3(3,4-dichlorophenyl)-1,1-dimethylurea; F_max ± Maximum yield of chlorophyll fluorescence - hr = hour - PAR = Photosynthetically Active Radiation - Q_A = Primary stable electron acceptor within photosystem II - qE = High energy state quenching of chlorophyll fluorescence - qI = quenching of chlorophyll fluorescence related to photoinhibition - qP = Quenching of chlorophyll fluorescence by oxidised plastoquinone - qQ = photochemical quenching of chlorophyll fluorescence - qR = (F_max—maximum level of chlorophyll fluorescence induced by the addition of saturating DCMU) - qT = Quenching of chlorophyll fluorescence attributable to state transitions     

Spectroscopic studies of interaction of chlorobenzylidine with DNA

Electronic absorbance and fluorescence titrations are used to probe the interaction of chlorobenzylidine with DNA. The binding of chlorobenzylidine to DNA results in hypochromism, a small shift to a longer wavelength in the absorption spectra, and emission quenching in the fluorescence spectra. These spectral characteristics suggest that chlorobenzylidine binds to DNA by an intercalative mode. This conclusion is reinforced by fluorescence polarization measurements. Scatchard plots constructed from fluorescence titration data give a binding constant of 1.3 x 10(5) M(-1) and a binding site size of 10 base pairs. This indicates that chlorobenzylidine has a high affinity with DNA. The intercalative interaction is exothermic with a Van't Hoff enthalpy of -143 kJ/mol. This result is obtained from the temperature dependence of the binding constant. The interaction of chlorobenzylidine with DNA is affected by the pH value of the solution. The binding constant has its maximum at pH 3.0. Upon binding to DNA, the fluorescence from chlorobenzylidine is quenched efficiently by the DNA bases and the fluorescence intensity tends to be constant at high concentrations of DNA when the binding is saturated. The Stern-Volmer quenching constant obtained from the linear quenching plot is 1.6 x 10(4) M(-1) at 25 degrees C. The measurements of the fluorescence lifetime and the dependence of the quenching constant on the temperature indicate that the fluorescence quenching process is static. The fluorescence lifetime of chlorobenzylidine is 1.9 +/- 0.4 ns.     

Induction of photochemical and non-photochemical quenching of chlorophyll fluorescence by low concentrations of m-dinitrobenzene

Chlorophyll fluorescence quenching induced by low concentrations of m-dinitrobenzene (DNB) is investigated. In intact spinach chloroplasts DNB causes photochemical and non-photochemical quenching. The two forms of quenching are distinguished by applying the saturation pulse method with a new type of modulation fluorometer. Half-maximal photochemical quenching is observed at about 3 micromolar DNB. It is inhibited by 3-(3,4 dichlorophenyl)-1, 1-dimethylurea (DCMU) and by 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone (DBMIB). Photochemical quenching by DNB leads to suppression of the I-P transient in a fluorescence induction curve. Upon application of saturating continuous light, the increase of fluorescence yield is separated into a photochemical and a thermal part. DNB causes suppression of only the slowest sub-component of the thermal part, in analogy to the action of Hill reagents. Simultaneous measurements of oxygen exchange rate and fluorescence reveal that a part of DNB induced quenching is accompanied by oxygen uptake. Most DNB-induced non-photochemical quenching is prevented by nigericin and, hence, can be considered energy-dependent quenching. The small component persisting in the presence of nigericin is identical to the one observed with methylviologen and other Hill reagents, likely to be due to static quenching by oxidized plastoquinone. The presented data confirm the original finding of Etienne and Lavergne (Biochim Biophys Acta 283: 268–278, 1972) that low concentrations of DNB selectively affect the thermal component of variable fluorescence. However, while these authors interpreted the quenching by a non-photochemical mechanism, the present investigation emphasizes a photochemical mechanism, in analogy to the effect of electron acceptors or mediators.Abbreviations DBMIB 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone - DCMU 3-(3,4-dichlorophenyl)-1, 1-dimethylurea - DNB m-dinitrobenzene - PGA 3-phosphoglycerate - PMS phenazinemethosulphate - PS I and PS II photosystems I and II     

Time-resolved fluorescence analysis of the photosystem II antenna proteins in detergent micelles and liposomes

We have studied the time-resolved fluorescence properties of the light-harvesting complexes (Lhc) of photosystem II (Lhcb) in order to obtain information on the mechanism of energy dissipation (non-photochemical quenching) which is correlated to the conversion of violaxanthin to zeaxanthin in excess light conditions. The chlorophyll fluorescence decay of Lhcb proteins LHCII, CP29, CP26, and CP24 in detergent solution is mostly determined by two lifetime components of 1.2-1.5 and 3.6-4 ns while the contribution of the faster component is higher in CP29, CP26, and CP24 with respect to LHCII. The xanthophyll composition of Lhc proteins affects the ratio of the lifetime components: when zeaxanthin is bound into the site L2 of LHCII, the relative amplitude of the faster component is increased and, consequently, the chlorophyll fluorescence quenching is enhanced. Analysis of quenching in mutants of Arabidopsis thaliana, which incorporate either violaxanthin or zeaxanthin in their Lhc proteins, shows that the extent of quenching is enhanced in the presence of zeaxanthin. The origin of the two fluorescence lifetimes was analyzed by their temperature dependence: since lifetime heterogeneity was not affected by cooling to 77 K, it is concluded that each lifetime component corresponds to a distinct conformation of the Lhc proteins. Upon incorporation of Lhc proteins into liposomes, a quenching of chlorophyll fluorescence was observed due to shortening of all their lifetime components: this indicates that the equilibrium between the two conformations of Lhcb proteins is displaced toward the quenched conformation in lipid membranes or thylakoids with respect to detergent solution. By increasing the protein density in the liposomes, and therefore the probability of protein-protein interactions, a further decrease of fluorescence lifetimes takes place down to values typical of quenched leaves. We conclude that at least two major factors determine the quenching of chlorophyll fluorescence in Lhcb proteins, i.e., intrasubunit conformational change and intersubunit interactions within the lipid membranes, and that these processes are both important in the photoprotection mechanism of nonphotochemical quenching in vivo.     

The effect of high-energy-state excitation quenching on maximum and dark level chlorophyll fluorescence yield

The quenching of variable fluorescence yield (q_N) and the quenching of dark level fluorescence yield (q₀) directly atributable to high-energy-state fluorescence quenching (q_E) was studied to distinguish between energy dissipation in the antenna and light harvesting complexes (antenna quenching) and energy dissipation at the reaction centres (reaction centre quenching). A consistent relationship was obtained between q_N and q₀ in barley leaves, the green alga Dunaliella C9AA and in pea thylakoids with 2,3,5,6-tetramethyl-p-phenylene diamine (DAD) as mediator of cyclic electron flow around PS 1. This correlated well with the relationship obtained using m-dinitrobenzene (DNB), a chemical model for antenna quenching, to quench fluorescence in Dunaliella C9AA or pea thylakoids. The results also correlated reasonably well with theoretical predictions by the Butler model for antenna quenching, but did not correlate with the predictions for reaction centre quenching. It is postulated that q_E quenching therefore occures in the antenna and light harvesting complexes, and that the small deviation from the Butler prediction is due to PS 2 heterogeneity.Abbreviations 9-aa 9-aminoacridine - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - EDTA Ethylenediaminetetra-acetic acid - Hepes 4-(2-hydroxyethyl)-1-piperazineethanesulphonic acid - Mes 2-(N-morpholino) prophanesulfonate - PS 1 photosystem 1 - PS 2 photosystem 2 - Q_A and Q_B primary and secondary stable electron acceptors of photosystem 2 - q_N non-photochemical fluorescence quenching coefficient - q_E high-energy-state fluorescence quenching coefficient - q₀ quenching coefficient for F₀ - F₀ dark level fluorescence yield - F_m maximum fluorescence yield - F_v variable fluorescence yield - F_v/F_m ratio of variable to total fluorescence yield - DAD 2,3,5,6-tetramethyl-p-phenylene diamine - DNB m-dinitrobenzene     

Aurovertin fluorescence changes of the mitochondrial F1-ATPase during multi- and uni-site ATP hydrolysis

The aurovertin-F1 complex was used to monitor fluorescence changes of the mitochondrial adenosine triphosphatase during multi- and uni-site ATP hydrolysis. It is known that the fluorescence intensity of the complex is partially quenched by addition of ATP or Mg2+ and enhanced by ADP (Chang, T., and Penefsky, H. S. (1973) J. Biol. Chem. 248, 2746-2754). In the present study low concentrations of ATP (0.03 mM) induced a marked fluorescence quenching which was followed by a fast fluorescence recovery. This recovery could be prevented by EDTA or an ATP regenerating system. The rate of ATP hydrolysis by the aurovertin-F1 complex and the reversal of the ATP-induced fluorescence quenching were determined in these various conditions. ITP hydrolysis also resulted in fluorescence quenching that was followed by a recovery of fluorescence intensity. Under conditions for single site catalysis, fluorescence quenching was observed upon the addition of ATP. This strongly indicates that fluorescence changes in the aurovertin-F1 complex are due to the binding and hydrolysis of ATP at a catalytic site. Therefore the resulting ADP molecule bound at this catalytic site possibly induces the fluorescence recovery observed.     

Electrical potential accelerates the E1P(Na)----E2P conformational transition of (Na,K)-ATPase in reconstituted vesicles

We have used renal (Na,K)-ATPase, covalently labeled with fluorescein, and phospholipid vesicles reconstituted with labeled enzyme, to detect conformational transitions induced by acetyl phosphate in the presence of Mg2+ and Na+ ions. Equilibrium fluorescence measurements show quenching of the fluorescein fluorescence, which is thought to reflect conversion of the initial E1 form to the phosphorylated E2P form. These fluorescence changes occur on inside-out-oriented pumps. The rates of acetyl phosphate-induced fluorescence changes have been measured using a stopped-flow fluorimeter. The rate of fluorescence quenching (1.5-3 s-1) is a measure of the rate of the E1P(Na)----E2P transition. The quenching is preceded by a fast fluorescence increase (12.3 +/- 4 s-1) associated with phosphorylation of E1 to E1P(Na), shown clearly in experiments with enzyme treated with oligomycin. Oligomycin greatly reduces the rate of the fluorescence quenching (0.044 +/- 0.01 s-1). Using potassium-loaded vesicles treated with valinomycin or lithium-loaded vesicles treated with Li+ ionophore N,N'-diheptyl-N,N'-didiethyl ether, 5,5-dimethyl-3,7-dioxanonanediamide in order to induce electrical diffusion potentials, negative inside, the rates of the fluorescence quenching are accelerated by up to 4-fold. The experiments demonstrate that the conformational transition E1P(Na)----E2P, associated with transport of 3 Na+ ions, is a voltage-sensitive reaction, carrying a net positive charge. This confirms a prediction based on transport experiments. In experiments with fluorescein-labeled (Na,K)-ATPase, the use of acetyl phosphate rather than ATP, which does not bind, provides a valuable tool to detect fluorescence signals accompanying steps in the turnover cycle.     

Synthesis and properties of fluorescent NF-kappa B-recognizing hairpin oligodeoxyribonucleotide decoys

Intramolecular fluorescence quenching of cyanine dyes was investigated using a model hairpin oligonucleotide decoy encoding a NF-kappaB p50 subunit binding site. Two types of hairpin oligonucleotides were synthesized: (1) 5'-(6-aminohexyl)- and 3'-(3-aminopropyl)-linked (I); (2) 5'-(6-aminohexyl)- and 3'-[3-(3-hydroxypropyldithio)propyl]-linked (II). Oligonucleotide I was covalently modified using monofunctional either Cy3- or Cy5.5-N-hydroxysuccinimide esters. Using reverse-phase HPLC, mono-and dicyanineamide derivatives of I were isolated. Mono-Cy3-modified derivatives of I, but not the mono-Cy5.5-modified derivatives, showed a 2-fold higher Cy3 fluorescence intensity compared to the free dye. There was no detectable difference in fluorescence between the di-Cy3 derivative of I and the free dye at the same concentration. However, there was a 4-fold quenching of fluorescence in the case of the di-Cy5.5 derivative of the same hairpin oligonucleotide. The quenching of Cy5.5 fluorescence could not be explained by the interaction of Cy5.5 with nucleotide bases as demonstrated by incubating free Cy5.5 dye with oligonuclotides. The quenching effect was further investigated using an oligonucleotide bearing a cleavable 3'-amino-terminated linker bearing an S-S bond (III). After modification of the 5'- and 3'-end of oligonucleotide III with a Cy5.5 monofunctional hydroxysuccinimide ester, a 70-75% quenching of fluorescence was observed. Fluorescence was 100% dequenched after the reduction of S-S bond. The obtained result unequivocally demonstrates that the formation of intramolecular Cy5.5 dimers is the dominant mechanism of fluorescence quenching in symmetric dye-dye hairpin decoy beacons.     

Slow fluorescence quenching of type A chloroplasts. Resolution into two components.

The divalent-cation-specific ionophore A23187 is used to define two components of the slow fluorescence quenching of type a spinach chloroplasts: ionophore-reversible and ionophore-resistant quenching. Ionophore-reversible quenching predominates at relatively low light intensities and approaches saturation as light levels are increased. It is sensitive to uncouplers and to 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) and is dark reversible. At high light intensities the bulk (greater than 80%) of slow fluorescence quenching is ionophore-resistant. Ionophore-resistant quenching is stimulated by carbonyl cyanide m-chlorophenyl hydrazone (CCCP) at pH 7.6 and by both CCCP and methylamine at pH 9.0. It is insensitive to DCMU and is not reversed in subsequent darkness. Taken together, the two components account for all quenching observed in Type A chloroplasts. Ionophore-reversible quenching is identified with the Mg2+-mediated fluorescence quenching described by Krause (Biochim. Biophys. Acta (1974) 333, 301-313) and by Barber and Telfer (in Membrane Transport in Plants (Dainty, J., AND Zimmermann, U., eds.), pp. 281-288, Springer-Verlag, Berlin, 1974). Ionophore-resistant quenching, a first-order process requiring high light, resembles the quenching reported by Jennings et al. (Biochim. Biophys. Acta (1976) 423, 264-274). The resolution of the fluorescence quenching phenomenon into two distinct components reconciles the apparently contradictory observations of these earlier investigations.     

Quenching of Chlorophyll a Fluorescence in Response to Na+-Dependent HCO3- Transport-Mediated Accumulation of Inorganic Carbon in the Cyanobacterium Synechococcus UTEX 625

In the cyanobacterium Synechococcus UTEX 625, the yield of chlorophyll a fluorescence decreased in response to the transport-mediated accumulation of intracellular inorganic carbon (CO2 + HCO3- + CO32- = dissolved inorganic carbon [DIC]) and subsequently increased to a near-maximum level following photosynthetic depletion of the DIC pool. When DIC accumulation was mediated by the active Na+-dependent HCO3- transport system, the initial rate of fluorescence quenching was found to be highly correlated with the initial rate of H14CO3- transport (r = 0.96), and the extent of fluorescence quenching was correlated with the size of the internal DIC pool (r = 0.99). Na+-dependent HCO3- transport-mediated accumulation of DIC caused fluorescence quenching in either the presence or absence of the CO2 fixation inhibitor glycolaldehyde, indicating that quenching was not due simply to NADP+ reduction. The concentration of Na+ required to attain one-half the maximum rate of H14CO3- transport, at 20 [mu]M external HCO3-, declined from 9 to 1 mM as the external pH increased from 8 to 9.6. A similar pH dependency was observed when fluorescence quenching was used to determine the kinetic constants for HCO3- transport. In cells capable of Na+-dependent HCO3- transport, both the initial rate and extent of fluorescence quenching increased with increasing external HCO3-, saturating at about 150 [mu]M. In contrast Na+-independent HCO3- transport-mediated fluorescence quenching saturated at an HCO3- concentration of about 10 [mu]M. It was concluded that measurement of chlorophyll a fluorescence emission provided a convenient, but indirect, means of following Na+-dependent HCO3- transport and accumulation in Synechococcus.     

Photochemical and Nonphotochemical Fluorescence Quenching Processes in the Diatom Phaeodactylum tricornutum

Nonphotochemical fluorescence quenching was found to exist in the dark-adapted state in the diatom Phaeodactylum tricornutum. Pretreatment of cells with the uncoupler carbonylcyanide m-chlorophenylhydrazone (CCCP) or with nigericin resulted in increases in dark-adapted minimum and maximum fluorescence yields. This suggests that a pH gradient exists across the thylakoid membrane in the dark, which serves to quench fluorescence levels nonphotochemically. The physiological processes involved in establishing this proton gradient were sensitive to anaerobiosis and antimycin A. Based on these results, it is likely that this energization of the thylakoid membrane is due in part to chlororespiration, which involves oxygen-dependent electron flow through the plastoquinone pool. Chlororespiration has been shown previously to occur in diatoms. In addition, we observed that cells treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea exhibited very strong nonphotochemical quenching when illuminated with actinic light. The rate and extent of this quenching were light-intensity dependent. This quenching was reversed upon addition of CCCP or nigericin and was thus due primarily to the establishment of a pH gradient across the thylakoid membrane. Preincubation of cells with CCCP or nigericin or antimycin A completely abolished this quenching. Cyclic electron transport processes around photosystem I may be involved in establishing this proton gradient across the thylakoid membrane under conditions where linear electron transport is inhibited. At steady state under normal physiological conditions, the qualitative changes in photochemical and nonphotochemical fluorescence quenching at increasing photon flux densities were similar to those in higher plants. However, important quantitative differences existed at limiting and saturating intensities. Dissimilarities in the factors that regulate fluorescence quenching mechanisms in these organisms may account for these differences.     

Observation and characterisation of a transient in the yield of chlorophyll fluorescence in intact spinach chloroplasts

A transient in chlorophyll fluorescence, which is associated with a transient in 9-aminoacridine fluorescence and a perturbation in the rate of oxygen evolution, has been observed in intact spinach chloroplasts. The results indicate that changes in the redox state of Q are, at least partially, responsible for the transient in chlorophyll fluorescence. The size of the transient is highly dependent upon the concentration of inorganic phosphate and upon the pH of the medium. The properties of the transient are consistent with the suggestion that it reflects changes in the levels of stromal intermediates during induction.Abbreviations BES NN-Bis(2-hydroxyethyl)2-aminoethanesulphonic acid dihydroxyacetone-P(DHAP): dihydroxyacetone phosphate glycerate-3-P (PGA): glycerate-3-phosphate - HEPES N-2-Hydroxyethylpiperazine-N-2-ethanesulphonic acid - MES 2-(N-Morpholino)ethanesulphonic acid - Pi inorganic phosphate - qE quenching of chlorophyll fluorescence by the energisation of the thylakoid membrane - qQ quenching of chlorophyll fluorescence by oxidised Q, the electron acceptor of photosystem 2 - ribose-5-P (R5P) ribose-5-phosphate - Rbu-5-P ribulose-5-phosphate     

Thermodynamics of the quenching of tyrosyl fluorescence by dithiothreitol

Tyrosyl fluorescence quenching by oxidized dithiothreitol (DTTo) in N-acetyl-L-tyrosine N'-methylamide, and native bovine pancreatic ribonuclease A and its reduced, S-methylated form, in aqueous solution is studied at pH 3.0. From the temperature dependence of the fluorescence quenching, it is demonstrated that the mechanism of the quenching process is probably static (formation of a complex), and not dynamic (collisional), in origin. Although other quenching mechanisms cannot be ruled out, our proposition that the quenching of tyrosyl fluorescence in these molecules is due to the formation of a complex between the tyrosyl moieties and DTTo is consistent with previously reported evidence indicating a strong tendency for aromatics to complex with various disulfide-containing compounds. The strength of binding is approximately the same for these three tyrosine-containing compounds, indicating that the microenvironments of their tyrosyl residues may be similar. With 1 M as the reference standard state, the following average thermodynamic parameters are established for the complexation (at 298 K): delta G0 = -3.32 kcal/mol, delta H0 = -1.1 kcal/mol, and delta S0 = 7.4 eu. The large positive value of delta S0 suggests that hydrophobic interactions may play an important role in the stabilization of such tyrosyl-disulfide complexes; the negative value of delta H0 suggests that polar interactions may also contribute to the formation of these complexes. Some possible implications with regard to protein-folding studies are discussed.     

Kinetic analysis of the interaction between amphotericin B and human serum albumin using surface plasmon resonance and fluorescence spectroscopy.

The binding interaction between amphotericin B and human serum albumin (HSA) has been studied using surface plasmon resonance (SPR) spectroscopy combined with a fluorescence quenching method to confirm the binding kinetic results. In this paper, the SPR method used to study the drug-protein interaction has been described in detail. The association rate constant, dissociation rate constant and the equilibrium association constant of amphotericin B binding to HSA were obtained using this method. To confirm the feasibility of the SPR method, a fluorescence quenching method was performed to obtain the equilibrium constant. In order to obtain more accurate results, experiment design was used to optimize the fluorescence quenching process. The two equilibrium association constants obtained using the two methods were 4.017 x 10(4) M(-1) (SPR) and 3.656 x 10(4) M(-1) (fluorescence quenching method) respectively.     

Photoinduced quenching of chlorophyll fluorescence in intact chloroplasts and algae. Resolution into two components

The light-induced decline of chlorophyll a fluorescence from a peak (P) to a low stationary level (S) in intact, physiologically active isolated chloroplasts and in intact Chlorella cells is shown to be predominantly composed of two components: (1) fluorescence quenching by partial reoxidation of the quencher Q, the primary acceptor of Photosystem II and (2) energy-dependent fluorescence quenching related to the photoinduced acidification of the intrathylakoid space. These two mechanisms of fluorescence quenching can be distinguished by the different kinetics of the relaxation of quenching observed upon addition of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea (DCMU). The relaxation of quenching by addition of DCMU is biphasic. The fast phase with a half-time of about 1 s is attributed to the reversal of Q-dependent quenching. The slow phase with a half-time of about 15 s in chloroplasts and 5 s in Chlorella cells is ascribed to relaxation of energy-dependent quenching. As shown by fluorescence spectroscopy at 77 K, the energy-dependent fluorescence quenching essentially is not caused by increased transfer of excitation energy to Photosystem I. By analyzing the energy- and Q-dependent components of quenching, information on the energy state of the thylakoid membranes and on the redox state of Q under various physiological conditions is obtained.     

Effect of phytohormones on the transmembrane translocation of protons in plasma membrane vesicles from tubers of Solanum tuberosum L

Effects of phytohormones gibberellic acid (GA) and abscisic acid (ABA) on the ATP-dependent transmembrane transport of protons were studied in plasma membrane vesicles (PMVs) from non-dormant potato tubers. The uptake of H+ into PMVs was assessed by the fluorescence quenching of acridine orange (AO) after the addition of ATP to the incubation medium. Addition of ATP to the incubation medium led to the instantaneous rise of the AO fluorescence intensity followed by its decrease. The fluorescence quenching was not observed in the presence of either protonophore CCCP or inhibitors of the membrane-bound H+-ATPase. It is concluded that the ATP-induced quenching of the AO fluorescence resulted from the accumulation of protons in PMVs due to the function of the plasma membrane-bound H+-ATPase. Depending on their concentrations, GA and ABA either inhibited or stimulated the ATP-driven H+ translocation across the vesicle membrane. The growth-stimulating hormone GA at concentrations of 10(-9)-10(-5) M increased the initial rate of the fluorescence quenching, whereas 10(-4) M GA slightly inhibited the H+ translocation. The growth inhibitor ABA at a concentration of 10(-9) M slightly increased the rate of the proton accumulation in PMVs; at higher concentrations (10(-8)-10(-4) M), ABA inhibited the H+ translocation. Acetic acid, which has pK similar to pK of GA and ABA, did not influence the ATP-dependent H+ accumulation in PMVs, suggesting the hormone-specific action of GA and ABA on the H+-ATPase activity. In the presence of DCC, which completely inhibited the accumulation of H+, GA and ABA did not affect the passive proton efflux from PMVs. It is proposed that the mechanisms of the regulatory effects of phytohormones may involve modification of H+-ATPase activity leading to changes in the electrochemical gradient of H+ across the plasma membrane.