Péter Maróti

Photoinhibition and law of reciprocity in photosynthetic reactions of Synechocystis sp. PCC 6803

Summary The effect of irradiance (neutron, alpha, X- and visible electromagnetic rays) on biological systems (survivals of organs, tissue cultures, breakage of DNA) has been widely studied in radiology. The biological effect of radiation depends on the dose (D = I · t; I and t are the intensity and time of irradiance, respectively). In photosynthesis light is a substrate for the photoelectronic conversion and can be toxic to photosystem II (PSII) as well. This toxicity is expressed by the degradation of the reaction centre D 1 protein and, as a consequence, the loss of PSII activity of wild type and mutant Synechocystis cells being subjected to high light. The aim of the present study was to examine whether the photoinhibition of PSII follows the reciprocity law characteristic of a dose response. We measured the change of steady state level of room temperature fluorescence at 685 nm (due to the antenna and reaction center chlorophylls), variable chlorophyll fluorescence and oxygen evolution of wild type Synechocystis 6803 cells after exposure to high light intensities (1200-8000 µmol · m -2 · s -1 ) for different durations (0-20 min). We observed that the log of degree of PSII inactivation as a function of light intensity gave a straight line, indicating the validity of the reciprocity law. Average cross-sectional areas for inactivation were found to be 0.066 m 2 /mol (steady state oxygen evolution), 0.12 m 2 /mol (steady state level of F 685nm ), and 0.25 m 2 /mol (induction of F v /F max ).

Photoinhibition of carotenoidless reaction centers from Rhodobacter sphaeroides by visible light. Effects on protein structure and electron transport

Inhibition of electron transport and damage to the protein subunits by visible light has been studied in isolated reaction centers of the non-sulfur purple bacterium Rhodobacter sphaeroides. Illumination by 1100 μEm−2 s−1 light induced only a slight effect in wild type, carotenoid containing 2.4.1. reaction centers. In contrast, illumination of reaction centers isolated from the carotenoidless R26 strain resulted in the inhibition of charge separation as detected by the loss of the initial amplitude of absorbance change at 430 nm arising from the P+QB− → PQB recombination. In addition to this effect, the L, M and H protein subunits of the R26 reaction center were damaged as shown by their loss on Coomassie stained gels, which was however not accompanied by specific degradation products. Both the loss of photochemical activity and of protein subunits were suppressed in the absence of oxygen. By applying EPR spin trapping with 2,2,6,6-tetramethylpiperidine we could detect light-induced generation of singlet oxygen in the R26, but not in the 2.4.1. reaction centers. Moreover, artificial generation of singlet oxygen, also led to the loss of the L, M and H subunits. Our results provide evidence for the common hypothesis that strong illumination by visible light damages the carotenoidless reaction center via formation of singlet oxygen. This mechanism most likely proceeds through the interaction of the triplet state of reaction center chlorophyll with the ground state triplet oxygen in a similar way as occurs in Photosystem II.

The IleL229 → Met mutation impairs the quinone binding to the QB-pocket in reaction centers of Rhodobacter sphaeroides

A spontaneous mutant (R/89) of photosynthetic purple bacterium Rhodobacter sphaeroides R-26 was selected for resistance to 200 μM atrazin. It showed increased resistance to interquinone electron transfer inhibitors of o-phenanthroline (resistance factor, RF=20) in UQo reconstituted isolated reaction centers and terbutryne in reaction centers (RF=55) and in chromatophores (RF=85). The amino acid sequence of the QB binding protein of the photosynthetic reaction center (the L subunit) was determined by sequencing the corresponding pufL gene and a single mutation was found (IleL229 → Met). The changed amino acid of the mutant strain is in van der Waals contact with the secondary quinone QB. The binding and redox properties of QB in the mutant were characterized by kinetic (charge recombination) and multiple turnover (cytochrome oxidation and semiquinone oscillation) assays of the reaction center. The free energy for stabilization of QAQB− with respect to QA−QB was ΔGAB=−60 meV and 0 meV in reaction centers and ΔGAB=−85 meV and −46 meV in chromatophores of R-26 and R/89 strains at pH 8, respectively. The dissociation constants of the quinone UQo and semiquinone UQo− in reaction centers from R-26 and R/89 showed significant and different pH dependence. The observed changes in binding and redox properties of quinones are interpreted in terms of differential effects (electrostatics and mesomerism) of mutation on the oxidized and reduced states of QB.

Quinone-dependent delayed fluorescence from the reaction center of photosynthetic bacteria.

Millisecond delayed fluorescence from the isolated reaction center of photosynthetic bacteria Rhodobacter sphaeroides was measured after single saturating flash excitation and was explained by thermal repopulation of the excited bacteriochlorophyll dimer from lower lying charge separated states. Three exponential components (fastest, fast, and slow) were found with lifetimes of 1.5, 102, and 865 ms and quantum yields of 6.4 x 10(-9), 2.2 x 10(-9), and 2.6 x 10(-9) (pH 8.0), respectively. While the two latter phases could be related to transient absorption changes, the fastest one could not. The fastest component, dominating when the primary quinone was prereduced, might be due to a small fraction of long-lived triplet states of the radical pair and/or the dimer. The fast phase observed in the absence of the secondary quinone, was sensitive to pH, temperature, and the chemical nature of the primary quinone. The standard free energy of the primary stable charge pair relative to that of the excited dimer was -910 +/- 20 meV at pH 8 and with native ubiquinone, and it showed characteristic changes upon pH and quinone replacement. The interaction energy ( approximately 50 meV) between the cluster of the protonatable groups around GluL212 and the primary semiquinone provides evidence for functional linkage between the two quinone binding pockets. An empirical relationship was found between the in situ free energy of the primary quinone and the rate of charge recombination, with practical importance in the estimation of the free energy levels from the easily available lifetime of the charge recombination. The ratio of the slow and fast components could be used to determine the pH dependence of the free energy level of the secondary stable charge pair relative to that of the excited dimer.

Coupling of cytochrome and quinone turnovers in the photocycle of reaction centers from the photosynthetic bacterium Rhodobacter sphaeroides

A minimal kinetic model of the photocycle, including both quinone (Q-6) reduction at the secondary quinone-binding site and (mammalian) cytochrome c oxidation at the cytochrome docking site of isolated reaction centers from photosynthetic purple bacteria Rhodobacter sphaeroides, was elaborated and tested by cytochrome photooxidation under strong continuous illumination. The typical rate of photochemical excitation by a laser diode at 810 nm was 2.200 s-1, and the rates of stationary turnover of the reaction center (one-half of that of cytochrome photooxidation) were 600 +/- 70 s-1 at pH 6 and 400 +/- 50 s-1 at pH 8. The rate of turnover showed strong pH dependence, indicating the contribution of different rate-limiting processes. The kinetic limitation of the photocycle was attributed to the turnover of the cytochrome c binding site (pH < 6), light intensity and quinone/quinol exchange (6 < pH < 8), and proton-coupled second electron transfer in the quinone acceptor complex (pH > 8). The analysis of the double-reciprocal plot of the rate of turnover versus light intensity has proved useful in determining the light-independent (maximum) turnover rate of the reaction center (445 +/- 50 s-1 at pH 7.8).

Early detection of mercury contamination by fluorescence induction of photosynthetic bacteria

The induction (sudden dark-to-light transition) of fluorescence of photosynthetic bacteria has proved to be sensitive tool for early detection of mercury (Hg(2+)) contamination of the culture medium. The major characteristics of the induction (dark, variable and maximum fluorescence levels together with rise time) offer an easier, faster and more informative assay of indication of the contamination than the conventional techniques. The inhibition of Hg(2+) is stronger in the light than in the dark and follows complex kinetics. The fast component (in minutes) reflects the damage of the quinone acceptor pool of the RC and the slow component (in hours) is sensitive to the disintegration of the light harvesting system including the loss of the structural organization and of the pigments. By use of fluorescence induction, the dependence of the diverse pathways and kinetics of the mercury-induced effects on the age and the metabolic state of the bacteria were revealed.

Key role of proline L209 in connecting the distant quinone pockets in the reaction center of Rhodobacter sphaeroides

Photosynthetic bacterial reaction centers convert light excitation into chemical free energy. The initial electron transfer leads to the consecutive semireductions of the primary (QA) and secondary (QB) quinone acceptors. The Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{A}^{-}}}\end{equation*}\end{document} and Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{B}^{-}}}\end{equation*}\end{document} formations induce proton uptake from the bulk. Their magnitudes (H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{A}^{-}}}\end{equation*}\end{document} and H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{B}^{-}}}\end{equation*}\end{document}, respectively) probe the electrostatic interactions within the complex. The pH dependence of H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{A}^{-}}}\end{equation*}\end{document} and H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{B}^{-}}}\end{equation*}\end{document} were studied in five single mutants modified at the L209 site (L209P→F,Y,W,E,T). This residue is situated at the border of a continuous chain of water molecules connecting QB to the bulk. In the wild type (WT), a proton uptake band is present at high pH in the H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{A}^{-}}}\end{equation*}\end{document} and H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{B}^{-}}}\end{equation*}\end{document} curves and is commonly attributed to a cluster of acidic groups situated nearby QB. In the H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{A}^{-}}}\end{equation*}\end{document} curves of the L209 variants, this band is systematically absent but remains in the H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{B}^{-}}}\end{equation*}\end{document} curves. Moreover, notable increase of H+/Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{B}^{-}}}\end{equation*}\end{document} is observed in the L209 mutants at neutral pH as compared with the WT. The large effects observed in all L209 mutants are not associated with significant structural changes (Kuglstatter, A., Ermler, U., Michel, H., Baciou, L. & Fritzsch, G. Biochemistry (2001) 40, 4253–4260). Our data suggest that, in the L209 mutants, the QB cluster does not respond to the Q\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \setlength{\oddsidemargin}{-69pt} \begin{document} \begin{equation*}{\mathrm{_{A}^{-}}}\end{equation*}\end{document} formation as observed in the WT. We propose that, in the mutants, removal of the rigid proline L209 breaks a necessary hydrogen bonding connection between the quinone sites. These findings suggest an important role for structural rigidity in ensuring a functional interaction between quinone binding sites.

Flash-induced proton transfer in photosynthetic bacteria.

A proton electrochemical potential across the membranes of photosynthetic purple bacteria is established by a light-driven proton pump mechanism: the absorbed light in the reaction center initiates electron transfer which is coupled to the vectorial displacement of protons from the cytoplasm to the periplasm. The stoichiometry and kinetics of proton binding and release can be tracked directly by electric (glass electrodes), spectrophotometric (pH indicator dyes) and conductimetric techniques. The primary step in the formation of the transmembrane chemiosmotic potential is the uptake of two protons by the doubly reduced secondary quinone in the reaction center and the subsequent exchange of hydroquinol for quinone from the membrane quinone-pool. However, the proton binding associated with singly reduced promary and/or secondary quinones of the reaction center is substoichiometric, pH-dependent and its rate is electrostatically enhanced but not diffusion limited. Molecular details of protonation are discussed based on the crystallographic structure of the reaction center of purple bacteriaRb. sphaeroides andRps. viridis, structure-based molecular (electrostatic) calculations and mutagenesis directed at protonatable amino acids supposed to be involved in proton conduction pathways.

INTENSITY AND TIME‐DEPENDENCE OF THE CAROTENOID TRIPLET QUENCHING UNDER LIGHT FLASHES OF RECTANGULAR SHAPE IN CHLORELLA

Abstract— As is known the chlorophyll fluorescence of photosynthetizing plants is strongly quenched by carotenoid triplet states if the exciting light intensity is high enough (> 10 kW/m2). This light‐induced quenching process was studied by measuring the relative yield of chlorophyll fluoresccncc excited with a pulsed argon laser at 20 C in light adapted algae as function of time (within lo μs) and exciting light intensity (<400 kW/m2). The experimental yield against time and yield against intensity curves have been adequately explained by a statistical model of Photosystem 2 (PS 2) units based upon the existence of freely moving excitons according to which the carotenoid triplet quenchers are randomly distributed and are perfect traps for excitons. Accepting the hypothesis that carotenoid triplet quenching occurs only in PS 2 units. it could be concluded that the height of the true zero level of PS 2 fluorescence is somewhat lower than the half value of the fluorescence level of the dark adapted state.

The local electric field within phospholipid membranes modulates the charge transfer reactions in reaction centres.

Three different cholesterol derivatives and phloretin, known to affect the local electric field in phospholipid membranes, have been introduced into Rhodobacter sphaeroides reaction centre-containing phospholipid liposomes. We show that cholesterol and 6-ketocholestanol significantly slow down the interquinone first electron transfer (approximately 10 times), whereas phloretin and 5-cholesten-3beta-ol-7-one leave the kinetics essentially unchanged. Interestingly, the two former compounds have been shown to increase the dipole potential, whereas the two latter decrease it. We also measured in isolated RCs the rates of the electron and proton transfers at the first flash. Over the pH range 7-10.5 both reactions display biphasic behaviors with nearly superimposable rates and amplitudes, suggesting that the gating process limiting the first electron transfer is indeed the coupled proton entry. We therefore interpret the effects of cholesterol and 6-ketocholestanol as due to dipole concentration producing an increased free energy barrier for protons to enter the protein perpendicular to the membrane. We also report for the first time in R. sphaeroides RCs, at room temperature, a biphasicity of the P(+)Q(A)(-) charge recombination, induced by the presence of cholesterol derivatives in proteoliposomes. We propose that these molecules decrease the equilibration time between two RC conformations, therefore revealing their presence.