The mechanism of cyclic electron flow.

Apart from the canonical light-driven linear electron flow (LEF) from water to CO2, numerous regulatory and alternative electron transfer pathways exist in chloroplasts. One of them is the cyclic electron flow around Photosystem I (CEF), contributing to photoprotection of both Photosystem I and II (PSI, PSII) and supplying extra ATP to fix atmospheric carbon. Nonetheless, CEF remains an enigma in the field of functional photosynthesis as we lack understanding of its pathway. Here, we address the discrepancies between functional and genetic/biochemical data in the literature and formulate novel hypotheses about the pathway and regulation of CEF based on recent structural and kinetic information.

Maximal cyclic electron flow rate is independent of PGRL1 in Chlamydomonas.

Cyclic electron flow (CEF) is defined as a return of the reductants from the acceptor side of Photosystem I (PSI) to the pool of its donors via the cytochrome b6f. It is described to be complementary to the linear electron flow and essential for photosynthesis. However, despite many efforts aimed to characterize CEF, its pathway and its regulation modes remain equivocal, and its physiological significance is still not clear. Here we use novel spectroscopic to measure the rate of CEF at the onset of light in the green alga Chlamydomonas reinhardtii. The initial redox state of the photosynthetic chain or the oxygen concentration do not modify the initial maximal rate of CEF (60 electrons per second per PSI) but rather strongly influence its duration. Neither the maximal rate nor the duration of CEF are different in the pgrl1 mutant compared to the wild type, disqualifying PGRL1 as the ferredoxin-plastoquinone oxidoreductase involved in the CEF mechanism.

Mechanism and analyses for extracting photosynthetic electrons using exogenous quinones - what makes a good extraction pathway?

Plants or algae take many benefits from oxygenic photosynthesis by converting solar energy into chemical energy through the synthesis of carbohydrates from carbon dioxide and water. However, the overall yield of this process is rather low (about 4% of the total energy available from sunlight is converted into chemical energy). This is the principal reason why recently many studies have been devoted to extraction of photosynthetic electrons in order to produce a sustainable electric current. Practically, the electron transfer occurs between the photosynthetic organism and an electrode and can be assisted by an exogenous mediator, mainly a quinone. In this regard, we recently reported on a method involving fluorescence measurements to estimate the ability of different quinones to extract photosynthetic electrons from a mutant of Chlamydomonas reinhardtii. In the present work, we used the same kind of methodology to establish a zone diagram for predicting the most suitable experimental conditions to extract photoelectrons from intact algae (quinone concentration and light intensity) as a function of the purpose of the study. This will provide further insights into the extraction mechanism of photosynthetic electrons using exogenous quinones. Indeed fluorescence measurements allowed us to model the capacity of photosynthetic algae to donate electrons to an exogenous quinone by considering a numerical parameter called "open center ratio" which is related to the Photosystem II acceptor redox state. Then, using it as a proxy for investigating the extraction of photosynthetic electrons by means of an exogenous quinone, 2,6-DCBQ, we suggested an extraction mechanism that was globally found consistent with the experimentally extracted parameters.

Rapid electron transfer to photosystem I and unusual spectral features of cytochrome c(6) in Synechococcus sp. PCC 7002 in vivo.

Cytochrome c(6) donates electrons to photosystem I (PS I) in Synechococcus sp. PCC 7002. In this work, we provide evidence for rapid electron transfer (t(1/2) = 3 micros) from cytochrome c(6) to PS I in this cyanobacterium in vivo, indicating prefixation of the reduced donor protein to the photosystem. We have investigated the cytochrome c(6)-PS I interaction by laser flash-induced spectroscopy of intact and broken cells and by redox titrations of membrane and supernatant fractions. Redox studies revealed the expected membrane-bound cytochrome f, b(6), and b(559) species and two soluble cytochromes with alpha-band absorption peaks of 551 and 553 nm and midpoint potentials of -100 and 370 mV, respectively. The characteristics and the symmetrical alpha-band spectrum of the latter correspond to typical cyanobacterial cytochrome c(6) proteins. Rapid oxidation of cytochrome c(6) by PS I in vivo results in a unique, asymmetric oxidation spectrum, which differs significantly from the spectra obtained for cytochrome c(6) in solution. The basis for the unusual cytochrome c(6) spectrum and possible mechanisms of cytochrome c(6) fixation to PS I are discussed. The occurrence of rapid electron transfer to PS I in cyanobacteria suggests that this mechanism evolved before the endosymbiotic origin of chloroplasts. Its selective advantage may lie in protection against photo-oxidative damage as shown for Chlamydomonas.

Site-directed mutations at D1-His198 and D2-His197 of photosystem II in Synechocystis PCC 6803: sites of primary charge separation and cation and triplet stabilization.

Site-directed mutations were introduced to replace D1-His198 and D2-His197 of the D1 and D2 polypeptides, respectively, of the photosystem II (PSII) reaction center of Synechocystis PCC 6803. These residues coordinate chlorophylls P(A) and P(B) which are homologous to the special pair Bchlorophylls of the bacterial reaction centers that are coordinated respectively by histidines L-173 and M-200 (202). P(A) and P(B) together serve as the primary electron donor, P, in purple bacterial reaction centers. In PS II, the site-directed mutations at D1 His198 affect the P(+)--P-absorbance difference spectrum. The bleaching maximum in the Soret region (in WT at 433 nm) is blue-shifted by as much as 3 nm. In the D1 His198Gln mutant, a similar displacement to the blue is observed for the bleaching maximum in the Q(y) region (672.5 nm in WT at 80 K), whereas features attributed to a band shift centered at 681 nm are not altered. In the Y(Z*)--Y(Z)-difference spectrum, the band shift of a reaction center chlorophyll centered in WT at 433--434 nm is shifted by 2--3 nm to the blue in the D1-His198Gln mutant. The D1-His198Gln mutation has little effect on the optical difference spectrum, (3)P--(1)P, of the reaction center triplet formed by P(+)Pheo(-) charge recombination (bleaching at 681--684 nm), measured at 5--80 K, but becomes visible as a pronounced shoulder at 669 nm at temperatures > or =150 K. Measurements of the kinetics of oxidized donor--Q(A)(-) charge recombination and of the reduction of P(+) by redox active tyrosine, Y(Z), indicate that the reduction potential of the redox couple P(+)/P can be appreciably modulated both positively and negatively by ligand replacement at D1-198 but somewhat less so at D2-197. On the basis of these observations and others in the literature, we propose that the monomeric accessory chlorophyll, B(A), is a long-wavelength trap located at 684 nm at 5 K. B(A)* initiates primary charge separation at low temperature, a function that is increasingly shared with P(A)* in an activated process as the temperature rises. Charge separation from B(A)* would be potentially very fast and form P(A)(+)B(A)(-) and/or B(A)(+)Pheo(-) as observed in bacterial reaction centers upon direct excitation of B(A) (van Brederode, M. E., et al. (1999) Proc. Natl. Acad Sci. 96, 2054--2059). The cation, generated upon primary charge separation in PSII, is stabilized at all temperatures primarily on P(A), the absorbance spectrum of which is displaced to the blue by the mutations. In WT, the cation is proposed to be shared to a minor extent (approximately 20%) with P(B), the contribution of which can be modulated up or down by mutation. The band shift at 681 nm, observed in the P(+)-P difference spectrum, is attributed to an electrochromic effect of P(A)(+) on neighboring B(A). Because of its low-energy singlet and therefore triplet state, the reaction center triplet state is stabilized on B(A) at < or =80 K but can be shared with P(A) at >80 K in a thermally activated process.

Coupling of electron and proton transfer in the photosynthetic water oxidase.

According to current estimates, the photosynthetic water oxidase functions with a quite restricted driving force. This emphasizes the importance of the catalytic mechanisms in this enzyme. The general problem of coupling electron and proton transfer is discussed from this viewpoint and it is argued that 'weak coupling' is preferable to 'strong coupling'. Weak coupling can be achieved by facilitating deprotonation either before (proton-first path) or after (electron-first path) the oxidation step. The proton-first path is probably relevant to the oxidation of tyrosine Y(Z) by P-680. Histidine D1-190 is believed to play a key role as a proton acceptor facilitating Y(Z) deprotonation. The pK(a) of an efficient proton acceptor is submitted to conflicting requirements, since a high pK(a) favors proton transfer from the donor, but also from the medium. H-bonding between Y(Z) and His, together with the Coulombic interaction between negative tyrosinate and positive imidazolium, are suggested to play a decisive role in alleviating these constraints. Current data and concepts on the coupling of electron and proton transfer in the water oxidase are discussed.

New insights on the proton pump associated with cytochrome b6f turnovers from the study of H/D substitution effects on the electrogenicity and electron transfer reactions.

We have studied the effect of protium/deuterium substitution on different kinetics associated with the turnovers of cytochrome b(6)f complex in whole cells of Chlamydomonas reinhardtii. Both the oxidation of cytochrome f and the reduction of hemes b were only little affected by the isotopic substitution. Contrasting with this, the initial slope of the electrogenic phase associated with cytochrome b(6)f turnover was slowed by a factor of 4 by H(2)O/D(2)O substitution. Whereas in the presence of H(2)O the electrogenic phase developed concomitantly with cytochrome b reduction, it lagged for a few hundreds of microseconds after cytochrome b reduction in the presence of D(2)O. We propose that a proton pump is triggered by the oxidation of plastoquinol at the Q(o) site. The proton transfer is specifically delayed upon isotopic substitution, accounting for the lack of significant effect on the electron-transfer reaction as well as for the strong decrease of the initial rate of the electrogenic phase.

A new electrochemical gradient generator in thylakoid membranes of green algae.

Using a new method of delayed luminescence digital imaging, mutants of Chlorella sorokiniana lacking the chloroplast CF0CF1 ATP synthase were isolated for the first time. Biochemical characterization of these strains indicates a lack of detectable synthesis and accumulation of the ATP synthase subunits alpha-CF1 and beta-CF1. Functional characterization indicates the presence of a permanent electrochemical gradient (DeltaMu) across the thylakoid membrane in the dark-adapted state, which is not suppressed under anaerobic conditions. Contrary to what is observed in the presence of the CF0CF1 ATP synthase, this gradient is essentially due to an electric field component DeltaPsi with no detectable DeltapH component, under both aerobic and anaerobic conditions. Neither the CF0CF1 ATP synthase nor a respiratory process can thus be responsible for a permanent gradient detected under these conditions. The previous proposal of a new ATP-dependent electrogenic pump in thylakoid membranes is supported by these results that, in addition, indicate a specificity of this new pump for ions other than protons.

Electrostatic interactions at the donor side of the photosynthetic reaction center of Rhodopseudomonas viridis.

The photosynthetic reaction center of Rhodopseudomonas viridis, a purple bacterium, contains a tetraheme cytochrome subunit. After its photoinduced oxidation, the primary donor, P, is reduced by the nearby heme (c559) of the tetraheme subunit in about 200 ns. This heme, in turn, is reduced by another heme (c556) of the subunit in about 2 micro(s). The midpoint potentials of P, c559, and c556 are known to be +500, +380, and +320 mV, respectively. The reduction kinetics of P+ are strongly biphasic in living cells, membrane fragments, and isolated reaction centers. We show here that this biphasicity reflects a small equilibrium constant (lower than 10) for the electron-transfer reaction between P and c559, which arises from a significant difference between the operating redox potentials of the P+/P and c559+/c559 couples and their equilibrium midpoint potentials. This difference is partly due to the effect of the permanent transmembrane potential, which arises from the cell metabolism, and to significant electrostatic interactions which develop between the electron carriers of the reaction center. Interestingly, the kinetic parameters of P+ reduction in decoupled cells or membrane fragments are identical to those reported for isolated reaction centers. We estimate an interaction of about 20 mV between c556 and c559 and about 90 mV between c559 and P. Consequently, the operating redox potential of the P+/P couple is 410 mV.

In vivo characterization of the electrochemical proton gradient generated in darkness in green algae and its kinetic effects on cytochrome b6f turnover.

When unicellular algal cells are placed under anaerobic conditions, a large electrochemical gradient is built in darkness across the thylakoid membranes. We have estimated, in vivo, the amplitude of the Delta pH component of this transmembrane potential and shown that the Delta pH is twice as large as the Delta Psi. The amplitude of the Delta mu tildeH+ (approximately 110-140 mV) fits well with estimations based on the ATP/ADP ratio measured in green algae under the same conditions, suggesting that an equilibrium state is established across the thylakoid membrane. Therefore, under anaerobic dark incubation of algae, the electrochemical transmembrane potential is determined only by the cellular ATP content. The existence of this Delta mu tildeH+ is expected to result in a constitutive amount of activated CFo-CF1 ATPase, thereby facilitating ATP synthesis under low light intensity illumination. We report also on the effects of this dark-existing electrochemical gradient on the cytochrome b6f complex turnover kinetics. We show that they are largely slowed by the presence of this electrochemical transmembrane potential. The pH component is mainly responsible for the kinetic slowing down of cytochrome b6f complex turnover, despite the fact that electrogenicity is associated with the reactions taking place within this complex. Therefore, in vivo, owing to the low lumenal pH, the oxidation of plastoquinol at the Qo site is limiting the turnover of the cytochrome b6f complex in the presence of the Delta pH, while in its absence the oxidation rate of the b6 hemes becomes rate-limiting.

Stabilization of charge separation and photochemical misses in photosystem II.

Illumination of photosystem II by a saturating short flash results in a stabilized charge separation in only about 90% of the reaction centers. During a series of flashes, the 10% fraction of "photochemical misses" is randomly redistributed among the centers. This phenomenon is investigated in DCMU-inhibited material, eliminating the contribution to misses due to electron transfer equilibrium on the quinone acceptors. Under such conditions, the miss coefficient is about 5% and is enhanced to about 40% in the presence of hydroxylamine at low pH. When a second flash is fired, its efficiency increases as a function of the time delay after the first flash (turnover experiments). This process involves three distinct time domains: <10 micros, 100 micros, and 10 ms. From a study of the 515-nm field-indicating change, it appears that the increased inefficiency caused by hydroxylamine is not due to a lesser amount of initial charge separation but to a recombination process concomitant with the 100 micros phase of the turnover. The slow turnover phase (10 ms) is not associated with a recombination or any other electron transfer event but reflects a modification of open centers during which their probability to achieve charge stabilization rather than recombination is progressively increased. These results are interpreted in terms of an equilibrium between two conformational states of the centers endowed with different stabilization yield ("good" and "bad " stabilizers). The 100 micros turnover phase is due to the reopening of the bad stabilizers by recombination, and the 10 ms phase accompanies the redistribution of these centers among the two conformational states.

Proton/hydrogen transfer affects the S-state-dependent microsecond phases of P680+ reduction during water splitting.

To investigate a possible coupling between P680+ reduction and hydrogen transfer, we studied the effects of H2O/D2O exchange on the P680+ reduction kinetics in the nano- and microsecond domains. We concentrated on studying the period-4 oscillatory (i.e., S-state-related) part of the reduction kinetics, by analyzing the differences between the P680+ reduction curves, rather than the full kinetics. Earlier observations that P680+ reduction kinetics have microsecond components were confirmed: the longest observable lifetime whose amplitude showed period-4 oscillations was 30 microseconds. We found that solvent isotope exchange left the nanosecond phases of the P680+ reduction unaltered. However, a significant effect on the oscillatory microsecond components was observed. We propose that, at least in the S0/S1 and S3/S0 transitions, hydrogen (proton) transfer provides an additional decrease in the free energy of the YZ+P680 state with respect to the YZP680+ state. This implies that relaxation of the state YZ+P680 is required for complete reduction of P680+ and for efficient water splitting. The kinetics of the P680+ reduction suggest that it is intraprotein proton/hydrogen rearrangement/transfer, rather than proton release to the bulk, which is occurring on the 1-30 microseconds time scale.

Function-directed mutagenesis of the cytochrome b6f complex in Chlamydomonas reinhardtii: involvement of the cd loop of cytochrome b6 in quinol binding to the Q(o) site.

The FUD2 mutant from the green alga Chlamydomonas reinhardtii expresses a cytochrome b6 variant of higher apparent molecular mass [Lemaire et al. (1986) Biochim. Biophys. Acta 851, 239-248]. Here, we show that the mutation corresponds to a 36 base pair duplication in the chloroplast petB gene, which corresponds to a 12 amino acid duplication in the cd loop of cytochrome b6. The resulting protein still binds its heme cofactors and assembles into cytochrome b6f complexes, which accumulate in wild type amounts in exponentially growing cells of FUD2. However, these cytochrome b6f complexes show loosened binding of the Rieske protein and are more prone to degradation in aging cells. Electron transfer through the cytochrome b6f complexes is about 8 times slower in FUD2 than in wild type cells. This is due to a slower oxidation of plastoquinol at the Q(o) site, the folding of which is most likely altered by the duplication. By varying the redox state of the plastoquinone pool in vivo, we show that there is a dramatic decrease in the affinity of the Q(o) site for plastoquinols, which is about 100 times lower in FUD2 than in wild type cells. Our results show that the value of the binding constant of plastoquinol to the Q(o) site (2 x 10(4) M(-1)) derived in [Kramer et al. (1994) Biochim. Biophys. Acta 1184, 251-262] may be extrapolated to in vivo conditions.

Charge recombination and proton transfer in manganese-depleted photosystem II.

The proton transfer reactions induced by the oxidation and reduction of the secondary donor, tyrosine YZ, have been studied in photosystem II after inactivation (Mn-depletion) of the oxygen-evolving complex. The rate of the recombination reaction of YZox with the reduced primary acceptor QA- appears modulated by a protonatable group with pK approximately 6 in the presence of YZox. The finding of monophasic recombination kinetics requires that the proton equilibration of this group is faster than the recombination rate. The same group modulates the extent of proton release, from 0 below pH 5 to 1 per center above pH 7. The kinetics of proton appearance and disappearance in the bulk medium are markedly dependent on the material used. In PSII core particles, the release is observed in the 100 micros range and the uptake accompanies the recombination reaction. In PSII membranes, both of these reactions are markedly delayed, so that the uptake considerably lags behind the completion of the recombination reaction. An electrochromic shift of a chlorophyll is present during the whole lifetime of YZox, suggesting a charged character of this species. A fast decreasing phase of this signal was observed in particles in the same time range as proton release. These results are discussed in the framework of a model where the proton originating from the formation of the neutral oxidized tyrosine radical (YZ.) remains locally trapped. In turn, this proton shifts the pK of a nearby group from a value >/=9 to a value of 6.

Isolation of a psaF-deficient mutant of Chlamydomonas reinhardtii: efficient interaction of plastocyanin with the photosystem I reaction center is mediated by the PsaF subunit.

The PsaF polypeptide of photosystem I (PSI) is located on the lumen side of the thylakoid membrane and its precise role is not yet fully understood. Here we describe the isolation of a psaF-deficient mutant of the green alga Chlamydomonas reinhardtii generated by co-transforming the nuclear genome of the cw15-arg7A strain with two plasmids: one harboring a mutated version of the psaF gene and the other containing the argininosuccinate lyase gene conferring arginine prototrophy. This psaF mutant still assembles a functional PSI complex and is capable of photoautotrophic growth. However, electron transfer from plastocyanin to P700+, the oxidized reaction center chlorophyll dimer, is dramatically reduced in the mutant, indicating that the PsaF subunit plays an important role in docking plastocyanin to the PSI complex. These results contrast with those obtained previously with a cyanobacterial psaF-, psaJ- double mutant where no phenotype was apparent.

Disseminated candidiasis, Candida arthritis, and unilateral skin lesions.

Candida species are the most common cause of systemic fungal infections in patients with hematologic malignancies. These infections are aggressive with rapid dissemination to various organs. Cutaneous lesions occur in 10% to 13% of cases, whereas Candida arthritis occurs infrequently. This report describes the first case of disseminated candidiasis in a patient with both Candida arthritis and unilateral cutaneous lesions.

Proton release during successive oxidation steps of the photosynthetic water oxidation process: stoichiometries and pH dependence.

Flash-induced absorption changes of pH-indicating dyes were investigated in photosystem II enriched membrane fragments, in order to retrieve the individual contributions to proton release of the successive transitions of the Kok cycle. These stoichiometric coefficients were found to be, in general, noninteger and to vary as a function of pH. Proton release on the S0----S1 step decreases from 1.75 at pH 5.5 to 1 at pH 8, while, on S1----S2 the stoichiometry increases from 0 to 0.5 in the same pH range and remains close to 1 for S2----S3. These findings are analyzed in terms of pK shifts of neighboring amino acid residues caused by electrostatic interactions with the redox centers involved in the two first transitions. The electrochromic shift of a chlorophyll, associated with the S transitions, responding to local electrostatic effects was investigated under similar conditions. The pH dependence of this signal upon the successive transitions was found correlated with the titration of the proton release stoichiometries, expressing the electrostatic balance between the oxidation and deprotonation processes.