Function of the polypeptides of the photosystem II reaction center in Chlamydomonas reinhardtii. Localization of the primary reactants

The distribution of the primary quinone and of the pheophytin acceptors has been studied in PS II particles isolated from Chlamydomonas reinhardtii, with respect to the distribution of the apoproteins of the two chlorophyll-protein complexes associated with the PS II core. We show that photoreduction of the primary quinone requires the presence of the 50 and 47 kDa polypeptides. On the contrary, charge separation between P-680 and the pheophytin acceptor molecules can occur within the chlorophyll-protein complex of which the 50 kDa polypeptide is the apoprotein. Functional analysis of the PS II fractions shows that an active PS II center contains one photoreducible quinone and one photoreducible pheophytin per 45 chlorophyll molecules. Stoichiometric analysis of the PS II fractions shows that a PS II reaction center contains 45 chlorophyll molecules associated with most likely one copy of the 50 kDa and the 47 kDa polypeptides.     

Excitation energy transfer and charge separation in the isolated Photosystem II reaction center

The nature of excitation energy transfer and charge separation in isolated Photosystem II reaction centers is an area of considerable interest and controversy. Excitation energy transfer from accessory chlorophyll a to the primary electron donor P680 takes place in tens of picoseconds, although there is some evidence that thermal equilibration of the excitation between P680 and a subset of the accessory chlorophyll a occurs on a 100-fs timescale. The intrinsic rate for charge separation at low temperature is accepted to be ca. (2 ps)^–1, and is based on several measurements using different experimental techniques. This rate is in good agreement with estimates based on larger sized particles, and is similar to the rate observed with bacterial reaction centers. However, near room temperature there is considerable disagreement as to the observed rate for charge separation, with several experiments pointing to a ca. (3 ps)^–1 rate, and others to a ca. (20 ps)^-1 rate. These processes and the experiments used to measure them will be reviewed.Abbreviations Chl chlorophyll - FWHM full-width at half-maximum - Pheo pheophytin - PS II Photosystem II - P680 primary electron donor of the Photosystem II reaction center - RC reaction center The US Government right to retain a non-exclusive, royalty free licence in and to any copyright is acknowledged.     

Mutation of the Chlamydomonas reinhardtii analogue of residue M210 of the Rhodobacter sphaeroides reaction center slows primary electron transfer in Photosystem II

Primary charge separation within Photosystem II (PS II) is much slower (time constant 21 ps) than the equivalent step in the related reaction center (RC) found in purple bacteria ( 3 ps). In the case of the bacterial RC, replacement of a specific tyrosine residue within the M subunit (at position 210 in Rhodobacter sphaeroides), by a leucine residue slows down charge separation to 20 ps. Significantly the analogous residue in PS II, within the D2 polypeptide, is a leucine not a tyrosine (at position D2-205, Chlamydomonas reinhardtii numbering). Consequently, it has been postulated [Hastings et al. (1992) Biochemistry 31: 7638–7647] that the rate of electron transfer could be increased in PS II by replacing this leucine residue with tyrosine. We have tested this hypothesis by constructing the D2-Leu205Tyr mutant in the green alga, Chlamydomonas reinhardtii, through transformation of the chloroplast genome. Primary charge separation was examined in isolated PS II RCs by time-resolved optical spectroscopy and was found to occur with a time constant of 40 ps. We conclude that mutation of D2-Leu205 to Tyr does not increase the rate of charge separation in PS II. The slower kinetics of primary charge separation in wild type PS II are probably not due to a specific difference in primary structure compared with the bacterial RC but rather a consequence of the P680 singlet excited state being a shallower trap for excitation energy within the reaction center.     

Kinetic and Energetic Model for the Primary Processes in Photosystem II

A detailed model for the kinetics and energetics of the exciton trapping, charge separation, charge recombination, and charge stabilization processes in photosystem (PS) II is presented. The rate constants describing these processes in open and closed reaction centers (RC) are calculated on the basis of picosecond data (Schatz, G. H., H. Brock, and A. R. Holzwarth. 1987. Proc. Natl. Acad. Sci. USA. 84:8414-8418) obtained for oxygen-evolving PS II particles from Synechococcus sp. with ~80 chlorophylls/P₆₈₀. The analysis gives the following results. (a) The PS II reaction center donor chlorophyll P₆₈₀ constitutes a shallow trap, and charge separation is overall trap limited. (b) The rate constant of charge separation drops by a factor of ~6 when going from open (Q-oxidized) to closed (Q-reduced) reaction centers. Thus the redox state of Q controls the yield of radical pair formation and the exciton lifetime in the Chl antenna. (c) The intrinsic rate constant of charge separation in open PS II reaction centers is calculated to be ~2.7 ps^-1. (d) In particles with open RC the charge separation step is exergonic with a decrease in standard free energy of ~38 meV. (e) In particles with closed RC the radical pair formation is endergonic by ~12 meV. We conclude on the basis of these results that the long-lived (nanoseconds) fluorescence generally observed with closed PS II reaction centers is prompt fluorescence and that the amount of primary radical pair formation is decreased significantly upon closing of the RC.     

The involvement of lipids in light-induced charge separation in the reaction center of photosystem II

Extraction of PS II particles with 50 mM cholate and 1 M NaCl releases several proteins (33-, 23-, 17- and 13 kDa) and lipids from the thylakoid membrane which are essential for O₂ evolution, dichlorophenolindophenol (DCIP) reduction and for stable charge separation between P680⁺ and Q_A ^-. This work correlates the results on the loss of steady-state rates for O₂ evolution and PS II mediated DCIP photo-reduction with flash absorption changes directly monitoring the reaction center charge separation at 830 nm due to P680⁺, the chlorophyll a donor. Reconstitution of the extracted lipids to the depleted membrane restores the ability to photo-oxidize P680 reversibly and to reduce DCIP, while stimulating O₂ evolution minimally. Addition of the extracted proteins of masses 33-, 23- and 17- kDa produces no further stimulation of DCIP reduction in the presence of an exogenous donor like DPC, but does enhance this rate in the absence of exogenous donors while also stimulating O₂ evolution. The proteins alone in the absence of lipids have little influence on charge separation in the reaction center. Thus lipids are essential for stable charge separation within the reaction center, involving formation of P680⁺ and Q_A ^-.Abbreviations A₈₃₀ Absorption change at 830 nm - Chl Chlorophyll - D₁ primary electron donor to P680 - DCIP 2,6-dichlorophenolindophenol - DPC 1,5-diphenylcarbazide - MOPS 3-(N-morpholino)propanesulfonic acid - P680 reaction center chlorophyll a molecule of photosystem II - PPBQ Phenyl-p-benzoquinone - PS II Photosystem II - Q_A, Q_B first and second quinone acceptors in PS II - V-DCIP rate of DCIP reduction - V-O₂ rate of oxygen evolution - Y water-oxidizing enzyme system - CHAPS 3-Cyclohexylamino-propanesulfonic acid     

Steps on the Way to Building Blocks,Topologies, Crystals and X-ray Structural Analysis of Photosystems I and II of Water-oxidizing Photosynthesis

Basic structural elements of the two photosystems and their component electron donors, acceptors, and carriers were revealed by newly developed spectroscopic methods in the 1960s and subsequent years. The spatial organization of these constituents within the functional membrane was elucidated by electrochromic band shift analysis, whereby the membrane-spanning chlorophyll-quinone couple of Photosystem (PS) II emerged as reaction center and as a model relevant also to other photosystems. A further step ahead for improved structural information was realized with the use of thermophilic cyanobacteria instead of plants which led to isolation of supramolecular complexes of the photosystems and their identification as PS I trimers and PS II dimers. The preparation of crystals of the PS I trimer, started in the late 1980s. Genes encoding the 11 subunits of PS I from Synechococcus elongatus were isolated and the predicted sequences of amino acid residues formed a basis for the interpretation of X-ray structure analysis of the PS I crystals. The crystallization of PS I was optimized by introduction of the 'reverse of salting in' crystallization with water as precipitating agent. On this basis the PS I structure was successively established from 6 A resolution in the early 1990s up to a model at 2.5 A resolution in 2001. The first crystals of the PS II dimer, capable of water oxidation, were prepared in the late 1990s; a PS II model at 3.8-3.6 A resolution was presented in 2001. Implications of the PS II structure for the mechanism of transmembrane charge separation are discussed. With the availability of PS I and PS II crystals, new directional structural results became possible also by application of different magnetic resonance techniques through measurements on single crystals in different orientations.     

Excitation energy transfer in intact cells and in the phycobiliprotein antennae of the chlorophyll d containing cyanobacterium Acaryochloris marina

The cyanobacterium Acaryochloris marina is unique because it mainly contains Chlorophyll d (Chl d) in the core complexes of PS I and PS II instead of the usually dominant Chl a. Furthermore, its light harvesting system has a structure also different from other cyanobacteria. It has both, a membrane-internal chlorophyll containing antenna and a membrane-external phycobiliprotein (PBP) complex. The first one binds Chl d and is structurally analogous to CP43. The latter one has a rod-like structure consisting of three phycocyanin (PC) homohexamers and one heterohexamer containing PC and allophycocyanin (APC). In this paper, we give an overview on the investigations of excitation energy transfer (EET) in this PBP-light-harvesting system and of charge separation in the photosystem II (PS II) reaction center of A. marina performed at the Technische Universität Berlin. Due to the unique structure of the PBP antenna in A. marina, this EET occurs on a much shorter overall time scale than in other cyanobacteria. We also briefly discuss the question of the pigment composition in the reaction center (RC) of PS II and the nature of the primary donor of the PS II RC.     

EPR signal II in cyanobacterial Photosystem II reaction-center complexes with and without the 40 kDa chlorophyll-binding subunit

The steady-state amplitude and flash-induced kinetics of EPR signal II in two Photosystem II (PS II) reaction center protein complexes from Synechococcus were measured to probe the organization of species involved in the PS II electron-transfer chain. A PS II reaction center complex (E-1) which has 47, 40, 31, 28 and 9 kDa subunits shows both fast decaying (signal II_f) and slowly decaying (signal II_s+u) EPR components. The amplitude of signal II_f, which represents Z (the donor to P-680), is about 1 spin per 30 Chl. This corresponds to one spin per reaction center in this preparation. Signal II_s+u, the slowly decaying component of signal II, reflects D, a donor to PS II on a side chain from the path of water oxidation in higher plants and algae. Signal II_s+u is present in the E-1 preparation in a ratio of about 1 spin per 40 Chl. Flash-induced signal II_f in E-1 shows biexponential decay with half-times of 20 ms and 300 ms. In a PS II reaction center complex (CP2b) which has 47, 31, 28 and 9 kDa subunits, but no 40 kDa subunit, an appreciable amount of signal II_f is observed (about 1 per 50 Chl). Less than 1 spin per 400 Chl of signal II_s+u is visible in this sample. The kinetics of Z⁺ reduction (signal II_f) in CP2b is similar to that seen in E-1 preparations, indicating that CP2b contains all of the molecules necessary for primary charge separation and secondary electron donation from Z.     

Defining the Far-red Limit of Photosystem I: THE PRIMARY CHARGE SEPARATION IS FUNCTIONAL TO 840 nm*

The far-red limit of photosystem I (PS I) photochemistry was studied by EPR spectroscopy using laser flashes between 730 and 850 nm. In manganese-depleted spinach thylakoid membranes, the primary donor in PS I, P₇₀₀, was oxidized simultaneously with tyrosine Z, the secondary donor in PS II. It was found that at 295 K PS I photochemistry, observed as P₇₀₀⁺ formation, was functional up to 840 nm. This is 30 nm further to the red region than was reported for PS II photochemistry (Thapper, A., Mamedov, F., Mokvist, F., Hammarström, L., and Styring, S. (2009) Plant Cell 21, 2391–2401). The same far-red limit for the P₇₀₀⁺ formation was observed in a PS I reaction center core preparation from Nostoc punctiforme. The reduction of the acceptor side of PS I, observed as reduction of the iron-sulfur centers F_A and F_B by low temperature EPR measurements, was also functional at 15 K with light up to >830 nm. Taken together, these results, obtained from both plants and cyanobacteria, most likely rule out involvement of the red-absorbing antenna chlorophylls in this reaction. Instead we propose the existence of weak charge transfer bands absorbing in the far-red region in the ensemble of excitonically coupled chlorophyll a molecules around P₇₀₀ similar to what has been found in the reaction center of PS II. These charge transfer bands could be responsible for the far-red light absorption leading to PS I photochemistry at wavelengths up to 840 nm.     

Photoelectric study on the kinetics of trapping and charge stabilization in oriented PS II membranes

Excitation energy trapping and charge separation in Photosystem II were studied by kinetic analysis of the fast photovoltage detected in membrane fragments from peas with picosecond excitation. With the primary quinone acceptor oxidized the photovoltage displayed a biphasic rise with apparent time constants of 100–300 ps and 550±50 ps. The first phase was dependent on the excitation energy whereas the second phase was not. We attribute these two phases to trapping (formation of P-680⁺ Phe^-) and charge stabilization (formation of P-680⁺ Q_A ^-), respectively. A reversibility of the trapping process was demonstrated by the effect of the fluorescence quencher DNB and of artificial quinone acceptors on the apparent rate constants and amplitudes. With the primary quinone acceptor reduced a transient photoelectric signal was observed and attributed to the formation and decay of the primary radical pair. The maximum concentration of the radical pair formed with reduced Q_A was about 30% of that measured with oxidized Q_A. The recombination time was 0.8–1.2 ns.The competition between trapping and annihilation was estimated by comparison of the photovoltage induced by short (30 ps) and long (12 ns) flashes. These data and the energy dependence of the kinetics were analyzed by a reversible reaction scheme which takes into account singlet-singlet annihilation and progressive closure of reaction centers by bimolecular interaction between excitons and the trap. To put on firmer grounds the evaluation of the molecular rate constants and the relative electrogenicity of the primary reactions in PS II, fluorescence decay data of our preparation were also included in the analysis. Evidence is given that the rates of radical pair formation and charge stabilization are influenced by the membrane potential. The implications of the results for the quantum yield are discussed.Abbreviations DCBQ 2,6-dichloro-p-benzoquinone - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - DNB m-dinitrobenzene - PPBQ phenyl-p-benzoquinone - PS I photosystem I of green plants - PS II photosystem II of green plants - PSU photosynthetic unit - P-680 primary donor of PS II - Phe intermediary pheophytin acceptor of PS II - Q_A primary quinone acceptor of PS II - RC reaction center     

In search of a putative long-lived relaxed radical pair state in closed photosystem II: Kinetic modeling of picosecond fluorescence data

The concept of a relaxed radical pair state in closed photosystem (PS) II centers (first quinone acceptor reduced) is critically examined on the basis of chlorophyll fluorescence decay data of the green alga Scenedesmus obliquus. Global analysis resulting in the decay-associated fluorescence spectra from closed PS II centers reveals a new PS II lifetime component (τ ≈ 380 ps) in addition to two PS II components (τ ~ 1.3 and 2.1 ns) resolved earlier. Particular emphasis was given to resolve a potential long-lived (~ 10 ns) component of small amplitude; however, the longest lifetime found is only 2.1 ns. From comparison of experimental and simulated data we conclude that the maximum relative amplitude of such a potential long-lived component must be <0.1%. The PS II kinetics are analyzed in terms of a three-state model involving an antenna/reaction center excited state, a primary radical pair state, and a relaxed radical pair state. The rate constants for charge separation and presumed radical pair relaxation as well as those for the reverse processes are calculated. Critical examination of these results leads us to exclude the formation with high yield (> 15%) of a long-lived (τ ≥ 3 ns) relaxed radical pair in closed PS II. If at all distinguishable kinetically and energetically from the primary radical pair, a relaxed radical pair would not live longer than 2-3 ns in green algae. The data suggest, however, that the concept of a long-lived relaxed radical pair state is inappropriate for intact PS II.     

Acceptor side photoinhibition in PS II: On the possible effects of the functional integrity of the PS II donor side on photoinhibition of stable charge separation

Photoinhibition under aerobic and anaerobic conditions was analyzed in O₂-evolving and in Tris-treated PS II-membrane fragments from spinach by measuring laser-flash-induced absorption changes at 826 nm reflecting the transient P680⁺ formation and the chlorophyll fluorescence lifetime. It was found that anaerobic photoinhibitory treatment leads in both types of samples to the appearence of two long-lived fluorescence components with lifetimes of 7 ns and 16 ns, respectively. The extent of these fluorescence kinetics depends on the state of the reaction center (open/closed) during the fluorescence measurements: it is drastically higher in the closed state. It is concluded that this long-lived fluorescence is mainly emitted from modified reaction centers with singly reduced Q_A(Q_A ^-). This suggests that the observation of long-lived fluorescence components cannot necessarily be taken as an indicator for reaction centers with missing or doubly reduced and protonated Q_A (Q_AH₂). Time-resolved measurements of 826 nm absorption changes show that the rate of photoinhibition of the stable charge separation (P680^*Q_A P680⁺Q_A ^-), is nearly the same in O₂-evolving and in Tris-treated PS II-membrane fragments. This finding is difficult to understand within the framework of the Q_AH₂-mechanism for photoinhibition of stable charge separation because in that case the rate of photoinhibition should strongly depend on the functional integrity of the donor side of PS II. Based on the results of this study it is inferred, that several processes contribute to photoinhibition within the PS II reaction center and that a mechanism which comprises double reduction and protonation of Q_A leading to Q_AH₂ formation is only of marginal – if any – relevance for photoinhibition of PS II under both, aerobic and anaerobic, conditions.     

Energy and electron transfer in photosystem II of a chlorophyll b-containing Synechocystis sp. PCC 6803 mutant

Using a Synechocystis sp. PCC 6803 mutant strain that lacks photosystem (PS) I and that synthesizes chlorophyll (Chl) b, a pigment that is not naturally present in the wild-type cyanobacterium, the functional consequences of incorporation of this pigment into the PS II core complex were investigated. Despite substitution of up to 75% of the Chl a in the PS II core complex by Chl b, the modified PS II centers remained essentially functional and were able to oxidize water and reduce Q(A), even upon selective excitation of Chl b at 460 nm. Time-resolved fluorescence decay measurements upon Chl excitation showed a significant reduction in the amplitude of the 60-70 ps component of fluorescence decay in open Chl b-containing PS II centers. This may indicate slower energy transfer from the PS II core antenna to the reaction center pigments or slower energy trapping. Chl b and pheophytin b were present in isolated PS II reaction centers. Pheophytin b can be reversibly photoreduced, as evidenced from the absorption bleaching at approximately 440 and 650 nm upon illumination in the presence of dithionite. Upon excitation at 685 nm, transient absorption measurements using PS II particles showed some bleaching at 650 nm together with a major decrease in absorption around 678 nm. The 650 nm bleaching that developed within approximately 10 ps after the flash and then remained virtually unchanged for up to 1 ns was attributed to formation of reduced pheophytin b and oxidized Chl b in some PS II reaction centers. Chl b-containing PS II had a lower rate of charge recombination of Q(A)(-) with the donor side and a significantly decreased yield of delayed luminescence in the presence of DCMU. Taken together, the data suggest that Chl b and pheophytin b participate in electron-transfer reactions in PS II reaction centers of Chl b-containing mutant of Synechocystis without significant impairment of PS II function.     

Characterization of the fast and slow reversible components of non-photochemical quenching in isolated pea thylakoids by picosecond time-resolved chlorophyll fluorescence analysis.

The fast and slow reversible components of non-photochemical chlorophyll fluorescence quenching commonly assigned to the qE and the qI mechanism have been studied in isolated pea thylakoids which were prepared from leaves after a moderate photoinhibitory treatment. Chlorophyll fluorescence decays were measured at picosecond resolution and analyzed on the basis of the heterogeneous exciton/radical pair equilibrium model. Our results show that the fast reversible non-photochemical quenching is completely assigned to the PS II antenna and is related to zeaxanthin. The slow reversible qI type quenching is located at the PS II reaction center and involves enhanced nonradiative decay of the primary charge separated state to its ground state and/or triplet excited state. Apart from its independence from the proton gradient, the qI quenching shows striking similarities to a particular form of qE quenching which is also located at the PS II reaction center and has resently been resolved in isolated thylakoids from dark-adapted leaves [Wagner, B., et al. (1996) J. Photochem. Photobiol., B 36, 339-350]. Our data suggest that during exposure to the supersaturating light the reaction center qE component was replaced by qI quenching. This qE to qI transition is supposed to be part of the mechanism of the long-term downregulation of PS II during photoinhibition. It is also evident that under the conditions used in our study zeaxanthin-dependent antenna quenching is not involved in the slow reversible downregulation of PS II but that it retains its dependence on the proton gradient during exposure to strong light.     

Isolation and Characterization of Photosystem Ⅱ Reaction Center D1-D2-Cytochrome b-559 Complex from the Chloroplasts of Spinach

Photosystem Ⅱ reaction center D1-D2-cytochrome b-559 pigment-protein complex has been isolated and purified from chloroplasts of spinach and its properties have been studied. The Isotared photosystem II reaction center contains close to six chlorophyll a per two pheophytin a molecules. Analysis of fluorescence decaying by phase modulation fluorometry suggests that the reaction center has three components of fluorescence decaying with lifetimes of 1.5 nS, 6.23 nS, 36.26 nS in terms of fractions to total fluorescence yield as 0.06, 0.67, 0.27 respectively. The ,6.25 nS fluorescence component corresponds to chlorophyll a which is energetically uncoupled from the process of charge separation. The proportion of 1.51 nS component is very low, and its source is unclear. The 36.25 nS fluorescence component is attributed to the recombination of the primary radical pair, and so represents the activity of charge separation.     

Inhibition of photosystem II of spinach by the respiration inhibitors piericidin A and thenoyltrifluoroacetone

The effects of several respiration inhibitors on photosystem II (PS II) were investigated. Among the agents tested, piericidin A and thenoyltrifluoroacetone (TTFA) inhibited the photosynthetic electron transport of spinach as measured from chlorophyll (Chl) fluorescence parameters (Fm'-F)/Fm' and Fv/Fm. Using specific donors and acceptors of electrons, we identified the sites of inhibition in and around the PS II complex; the site of inhibition by TTFA was between QA, primary quinone acceptor in PS II, and QB, secondary quinone acceptor, in the acceptor side of P680, the reaction center Chl of PS II, while inhibition by piericidin A of the acceptor side was downstream of Q(B), out of the PS II complex. Both agents also inhibited the donor side of P680, probably between tyrosine-161 of the reaction center protein of PS II and P680.     

Molecular Sizes of the Catalytic Units of Oxygen Evolution and the Reaction Center in Photosystem II of Spinach Thylakoids

Target analysis of the PS II reaction in spinach thylakoidsshowed that the respective molecular masses of the catalyticunits for oxygen evolution and the reaction center are about120 kDa and 250 kDa based on a kinetic separation of the tworeaction rates. The size of the oxygen-evolving enzyme agreedwith that determined for the PS II preparation from a thermophiliccyanobacterium by the same means [Nugent and Atkinson (1984)FEBS Lett. 170: 89]. Single hit-inactivation of oxygen evolutionand the PS II reaction center units indicates that each functionis driven by a structurally assembled unit. (Received August 6, 1984; Accepted December 17, 1984)     

Mechanisms of chlorophyll fluorescence revisited: Prompt or delayed emission from photosystem II with closed reaction centers?

This paper proposes a model which correlates the exciton decay kinetics observed in picosecond fluorescence studies with the primary processes of charge separation in the reaction center of photosystem II. We conclude that the experimental results from green algae and chloroplasts from higher plants are inconsistent with the concept that delayed luminescence after charge recombination should account for the long-lived (approx. 2 ns) fluorescence decay component of closed photosystem II centers. Instead, we show that the experimental data are in agreement with a model in which the long-lived fluorescence is also prompt fluorescence. The model suggests furthermore that the rate constant of primary charge separation is regulated by the oxidation state of the quinone acceptor Q_A.