The rate of charge recombination in Photosystem II

Loss by recombination of the charge separated state P₆₈₀⁺Q_A⁻ limits the performance of Photosystem II (PS II) as a photochemical energy converter. Time constants reported in literature for this process are mostly either near 0.17 ms or near 1.4 ms. The shorter time is found in plant PS II when reduction of P₆₈₀⁺ by the secondary electron donor Tyrosine Z cannot occur because Y_Z is already oxidized. The 1.4 ms recombination is seen in Y_Z-less mutants of the cyanobacterium Synechocystis. However, the rate of P₆₈₀⁺Q_A⁻ recombination that actually competes with the stabilization of the charge separation has not been previously reported. We have measured the kinetics of the flash-induced fluorescence yield changes in the microsecond time domain in Tris-washed spinach chloroplasts. In this way the kinetics and yield of P₆₈₀⁺ reduction by Y_Z were obtained, and the rate of the competing P₆₈₀⁺Q_A⁻ recombination could be evaluated. The recombination time was less than 0.5 ms; the best-fitting time constant was 0.1 ms. The presence of Y_Z^ox slightly decreased the efficiency of excitation trapping but did not seem to accelerate P₆₈₀⁺Q_A⁻ recombination. The two P₆₈₀⁺Q_A⁻ lifetimes in the literature probably reflect a significant difference between plant and cyanobacterial PS II.     

Photosystem II electron transfer cycle and chlororespiration in planktonic diatoms

The dominance of diatoms in turbulent waters suggests special adaptations to the wide fluctuations in light intensity that phytoplankton must cope with in such an environment. Our recent demonstration of the unusually effective photoprotection by the xanthophyll cycle in diatoms [Lavaud et al. (2002) Plant Physiol 129 (3) (in press)] also revealed that failure of this protection led to inactivation of oxygen evolution, but not to the expected photoinhibition. Photo-oxidative damage might be prevented by an electron transfer cycle around Photosystem II (PS II). The induction of such a cycle at high light intensity was verified by measurements of the flash number dependence of oxygen production in a series of single-turnover flashes. After a few minutes of saturating illumination, the oxygen flash yields are temporarily decreased. The deficit in oxygen production amounts to at most 3 electrons per PS II, but continues to reappear with a half time of 2 min in the dark until the total pool of reducing equivalents accumulated during the illumination has been consumed by (chloro)respiration. This is attributed to an electron transfer pathway from the plastoquinone pool or the acceptor side of PS II to the donor side of PS II that is insignificant at limiting light intensity but is accelerated to milliseconds at excess light intensity. Partial filling of the 3-equivalents capacity of the cyclic electron transfer path in PS II may prevent both acceptor-side photoinhibition in oxygen-evolving PS II and donor-side photoinhibition when the oxygen-evolving complex is temporarily inactivated. This revised version was published online in June 2006 with corrections to the Cover Date.     

Regulation of Photosystem I electron flow activity by phosphatidylglycerol in thylakoid membranes as revealed by phospholipase treatment

Thylakoid membranes were treated by potato lipolytic acyl hydrolase, phospholipases A₂ from pancreas and snake venom, and by phospholipase C from Bacillus cereus under various conditions. The changes in the uncoupled rates of electron transport through Photosystem I (PS I) and in lipid composition were followed during these treatments. Pancreatic phospholipase A₂ which destroyed all phospholipids in thylakoid membranes stimulated the NADP⁺ reduction supported by reduced 2,6-dichlorophenolindophenol. This stimulation concerned only the dark but not the light reactions of this pathway. The main site of action of pancreatic phospholipase A₂ may be located on the donor side of PS I; the hydrolysis of phospholipids at this site caused an increased ability of reduced 2,6-dichlorophenolindophenol and ascorbate alone to feed electrons into PS I. A second site may be located on the acceptor side of PS I, probably between the primary acceptor and the ferredoxin system. When thylakoid membranes were first preincubated with or without lipolytic acyl hydrolase at 30°C (pH 8), the NADP⁺ photoreduction was inhibited whilst the methyl viologen-mediated O₂ uptake was stimulated. A subsequent addition of pancreatic phospholipase A₂ (which had the same hydrolysis rates for phosphatidylglycerol but not for phosphatidylcholine) further stimulated the O₂ uptake and restored NADP⁺ photoreduction. The extent of this stimulation, which depended on the presence of lipolytic acyl hydrolase, was ascribed partly to the hydrolysis of the phospholipids and partly to the generation of their lyso derivatives but not to the release of free fatty acids. On the contrary, phospholipase C which destroyed only phosphatidylcholine failed to restore this activity. It is suggested that phosphatidylglycerol is the only phospholipid associated with thylakoid membrane structures supporting PS I activities and that this lipid may play a physiological role in the regulation of these activities.     

The essential role of phosphatidylglycerol in photosynthesis

Since the first identification of phosphatidylglycerol in Scenedesmus by Benson and Maruo in 1958, researchers have studied many biological functions of this phospholipid. Genetic, biochemical, and structural studies of photosynthetic organisms have revealed that phosphatidylglycerol is crucial to the photosynthetic transport of electrons, the development of chloroplasts, and tolerance to chilling. In this review, we summarize our present understanding of the biochemical and physiological functions of phosphatidylglycerol in cyanobacteria and higher plants. Submitted to the special issue in honor of Andrew A. Benson     

Roles of the acidic lipids sulfoquinovosyl diacylglycerol and phosphatidylglycerol in photosynthesis: their specificity and evolution

Sulfoquinovosyl diacylglycerol (SQDG) and phosphatidylglycerol (PG) are lipids with negative charges, distributed among membranes of chloroplasts of plants and their postulated progenitors, cyanobacteria, and also widely among membranes of anoxygenic photosynthetic bacteria. Thus, these acidic lipids are of great interest in terms of their roles in the function and evolution of the photosynthetic membranes. The physiological significance of these lipids in photosynthesis has been examined through characterization of mutants defective in their abilities to synthesize SQDG or PG, and through characterization of isolated thylakoid membranes or photosynthetic particles, the acidic lipid contents of which were manipulated in vitro, for example, on treatment with phospholipase to degrade PG. Responsibility of SQDG or PG has been clarified so far in terms of the structural and/or functional integrity of photosystems I and/or II in cyanobacterial, green algal, and higher plant species. Also implied were distinct levels of the responsibility in the different photosynthetic organisms. Extreme cases involved the indispensability of SQDG for photosynthesis and growth in two prokaryotic, photosynthetic organisms and the contribution of PG to construction of the photosystem-I trimer exclusively in cyanobacteria. Here, roles of these acidic lipids are discussed with a focus on their specificity and the evolution of photosynthetic membranes.Norihiro Sato is the recipient of the Botanical Society Award for Young Scientist, 2003.     

Inhibition of Photosystem II activity by saturating single turnover flashes in calcium-depleted and active Photosystem II

Inhibition of Photosystem II (PS II) activity induced by continuous light or by saturating single turnover flashes was investigated in Ca²⁺-depleted, Mn-depleted and active PS II enriched membrane fragments. While Ca²⁺- and Mn-depleted PS II were more damaged under continuous illumination, active PS II was more susceptible to flash-induced photoinhibition. The extent of photoinactivation as a function of the duration of the dark interval between the saturating single turnover flashes was investigated. The active centres showed the most photodamage when the time interval between the flashes was long enough (32 s) to allow for charge recombination between the S₂ or S₃ and Q_B ⁻ to occur. Illumination with groups of consecutive flashes (spacing between the flashes 0.1 s followed by 32 s dark interval) resulted in a binary oscillation of the loss of PS II-activity in active samples as has been shown previously (Keren N, Gong H, Ohad I (1995), J Biol Chem 270: 806–814). Ca²⁺- and Mn-depleted PS II did not show this effect. The data are explained by assuming that charge recombination in active PS II results in a back reaction that generates P₆₈₀ triplet and thence singlet oxygen, while in Ca²⁺- and Mn-depleted PS II charge recombination occurs through a different pathway, that does not involve triplet generation. This correlates with an up-shift of the midpoint potential of Q_A in samples lacking Ca²⁺ or Mn that, in term, is predicted to result in the triplet generating pathway becoming thermodynamically less favourable (G.N. Johnson, A.W. Rutherford, A. Krieger, 1995, Biochim. Biophys. Acta 1229, 201–207). The diminished susceptibility to flash-induced photoinhibition in Ca²⁺- and Mn-depleted PS II is attributed at least in part to this mechanism. This revised version was published online in June 2006 with corrections to the Cover Date.     

Mathematical modelling of the light response curve of photoinhibition of Photosystem II

The light response curves of the acceptor and donor side mechanisms of photoinhibition of Photosystem II were calculated, using Arabidopsis as a model organism. Acceptor-side photoinhibition was modelled as double reduction of Q_A, noting that non-photochemical quenching has the same effect on the quantum yield of Q_A double reduction in closed PSII centres as it has on the quantum yield of electron transport in open centres. The light response curve of acceptor-side photoinhibition in Arabidopsis shows very low efficiency under low intensity light and a relatively constant quantum yield above light saturation of photosynthesis. To calculate the light response curve of donor-side photoinhibition, we built a model describing the concentration of the oxidized primary donor P₆₈₀⁺ during steady-state photosynthesis. The model is based on literature values of rate constants of electron transfer reactions of PSII, and it was fitted with fluorescence parameters measured in the steady state. The modelling analysis showed that the quantum yield of donor-side photoinhibition peaks under moderate light. The deviation of the acceptor and donor side mechanisms from the direct proportionality between photoinhibition and photon flux density suggests that these mechanisms cannot solely account for photoinhibition in vivo, but contribution of a reaction whose quantum yield is independent of light intensity is needed. Furthermore, a simple kinetic calculation suggests that the acceptor-side mechanism may not explain singlet oxygen production by photoinhibited leaves. The theoretical framework described here can be used to estimate the yields of different photoinhibition mechanisms under different wavelengths or light intensities.     

Interaction of 1,4-benzoquinones with Photosystem II in thylakoids and Photosystem II membrane fragments from spinach

The interaction of exogenous quinones with the Photosystem II (PS II) acceptor side has been analyzed by measurements of flash-induced 320 nm absorption changes, transient flash-induced variable fluorescence changes, thermoluminescence emission and oxygen yield in dark-adapted thylakoids and PS II membrane fragments. Two classes of 1,4-benzoquinones were shown to give rise to remarkably different reaction patterns. (A) Phenyl-p-benzoquinone (Ph-p-BQ) -type compounds give rise to a marked binary oscillation of the initial amplitudes of 320 nm absorption changes induced by a flash train in dark-adapted PS II membrane fragments and a retardation of the decay kinetics of the flash-induced variable fluorescence. The electron transfer reactions to these type of quinones are severely inhibited by 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU). (B) In the presence of tribromotoluquinone (TBTQ) a different oscillation pattern of the 320 nm absorption changes is observed characterized by a marked relaxation after the first flash in the 5 ms domain. This relaxation is insensitive to 10 μM DCMU. Likewise the decay of the flash-induced variable fluorescence in TBTQ-treated samples is much less sensitive to DCMU than in control. The thermoluminescence emission exhibits an oscillation in samples incubated for 5 min with TBTQ before addition of 30 μM DCMU. Under the same conditions a significant flash-induced oxygen evolution is observed only after the third and fourth flash, respectively, whereas in the presence of TBTQ alone a normal oscillation pattern is observed. The different functional patterns of PS II caused by the two types of classes of exogenous quinones are interpreted by their binding properties: a noncovalent association with the Q_B-site of Ph-p-BQ-type quinones versus a tight (covalent?) binding in the vicinity of Q_A (possibly also at the Q_B-site) in the case of halogenated 1,4-benzoquinones. The mechanistic implications of these findings are discussed.     

The PsbZ subunit of Photosystem II in Synechocystis sp. PCC 6803 modulates electron flow through the photosynthetic electron transfer chain

The psbZ gene of Synechocystis sp. PCC 6803 encodes the ∼6.6 kDa photosystem II (PSII) subunit. We here report biophysical, biochemical and in vivo characterization of Synechocystis sp. PCC 6803 mutants lacking psbZ. We show that these mutants are able to perform wild-type levels of light-harvesting, energy transfer, PSII oxygen evolution, state transitions and non-photochemical quenching (NPQ) under standard growth conditions. The mutants grow photoautotrophically; however, their growth rate is clearly retarded under low-light conditions and they are not capable of photomixotrophic growth. Further differences exist in the electron transfer properties between the mutants and wild type. In the absence of PsbZ, electron flow potentially increased through photosystem I (PSI) without a change in the maximum electron transfer capacity of PSII. Further, rereduction of P700⁺ is much faster, suggesting faster cyclic electron flow around PSI. This implies a role for PsbZ in the regulation of electron transfer, with implication for photoprotection.     

Afterglow thermoluminescence band as a possible early indicator of changes in the photosynthetic electron transport in leaves

The afterglow (AG) band of thermoluminescence (TL) has been investigated in leaves of Arabidopsis thaliana. Excitation of dark-adapted leaves with two saturating single turn-over flashes induced the appearance of a complex TL glow curve that could be well simulated by three components: the two components, B₁ and B₂, of the usually called B-band, peaking at 18 and 26 °C, respectively, and a band with t_max at 41 °C, which we attributed to an AG emission. Illumination of dark-adapted leaves with 720 nm monochromatic and FR lights generated the emission of a sharp single band peaking also around at 41 °C, that it is usually assigned to an AG emission band. Dark-incubation of whole plants increased the intensity of AG-band in TL curves induced by two flashes and, in parallel, decreased B-bands. Selective illumination of leaves with light mostly absorbed by PS II (650 nm light) completely abolished the AG-band induced by two flashes, B-band being the only TL band observed. The single AG-band induced by 720 nm light was abolished if leaves were also illuminated with 650 nm light. On the other hand, AG-band could be restored if 650 nm illuminated leaves were afterwards illuminated with 720 nm light. The changes in the intensity of B and AG bands induced by selective illuminations seem to be related to alterations in the redox state of Q_B and plastoquinone pool.     

Effect of monochromatic UV-B radiation on electron transfer reactions of Photosystem II

The adverse effect of low intensity, small band UV-B irradiation (λ = 305 ± 5 nm, I = 300 mW m⁻²) on PS II has been studied by comparative measurements of laser flash-induced changes of the absorption at 325 nm, ΔA₃₂₅(t), as an indicator of redox changes in Q_A, and of the relative fluorescence quantum yield, F(t)/F_o, in PS II membrane fragments. The properties of untreated control were compared with those of samples where the oxygen evolution rate under illumination with continuous saturating light was inhibited by up to 95%. The following results were obtained: a) the detectable initial amplitude (at a time resolution of 30 μs) of the 325 nm absorption changes, ΔA₃₂₅, remained virtually invariant whereas the relaxation kinetics exhibit significant changes, b) the 300 μs kinetics of ΔA₃₂₅ dominating the relaxation in UV-B treated samples was largely replaced by a 1.3 ms kinetics after addition of MnCl₂, c) the extent of the flash induced rise of the relative fluorescence quantum yield was severely diminished in UV-B treated PS II membrane fragments but the relaxation kinetics remain virtually unaffected. Based on these results the water oxidizing complex (WOC) is inferred to be the primary target of UV-B impairment of PS II while the formation of the ‘stable’ radical pair P680^+·Q_A ^−● is almost invariant to this UV-B treatment. This revised version was published online in June 2006 with corrections to the Cover Date.     

Functional size of Photosystem II determined by radiation inactivation

The functional size of Photosystem II (PS II) was investigated by radiation inactivation. The technique provides an estimate of the functional mass required for a specific reaction and depends on irradiating samples with high energy -rays and assaying the remaining activity. The analysis is based on target theory that has been modified to take into account the temperature dependence of radiation inactivation of proteins. Using PS II enriched membranes isolated from spinach we determined the functional size of primary charge separation coupled to water oxidation and quinone reduction at the Q_B site: H₂O (Mn)₄ Y_z P680 Pheophytin Q phenyl-p-benzoquinone. Radiation inactivation analysis indicates a functional mass of 88 ± 12 kDa for electron transfer from water to phenyl-p-benzoquinone. It is likely that the reaction center heterodimer polypeptides, D1 and D2, contribute approximately 70 kDa to the functional mass, in which case polypeptides adding up to approximately 20 kDa remain to be identified. Likely candidates are the and subunits of cytochrome b ₅₅₉and the 4.5 kDa psbI gene product.Abbreviations Cyt cytochrome - PS Photosystem - P680 primary electron donor of Photosystem II - Q_A primary quinone acceptor of Photosystem II - Q_B secondary quinone acceptor of Photosystem II - Y_z tyrosine donor to P680     

Engineering model proteins for Photosystem II function

Our knowledge of Photosystem II and the molecular mechanism of oxygen production are rapidly advancing. The time is now ripe to exploit this knowledge and use it as a blueprint for the development of light-driven catalysts, ultimately for the splitting of water into O₂ and H₂. In this article, we outline the background and our approach to this technological application through the reverse engineering of Photosystem II into model proteins.     

Purification of a Photosystem II reaction center from a thermophilic cyanobacterium using immobilized metal affinity chromatography

Oxygen-evolving PS II particles from the thermophilic cyanobacterium Synechococcus elongatus are partially purified by centrifugation on a sucrose gradient and are bound to a Chelating Sepharose column loaded with Cu²⁺ ions. Bound particles are then transformed into PS II RC complexes by two washing steps. First, washing with a phosphate buffer (pH=6.5) containing 0.02% of SB 12 removes the rest of phycobilins and leaves pure PS II core particles on the column. Second, washing with a phosphate buffer (pH=6.2) containing 0.2 M LiClO₄ and 0.05% of DM removes CP 47 and CP 43 and leaves bare PS II RC complexes on the column. These are then eluted with a phosphate buffer containing 1% of dodecylmaltoside (DM). The molar ratio of pigments in the eluate changes with the progress of elution but around the middle of the elution period a nearly stable ratio is maintained of Chl a: Pheo a: Car: Cyt b 559 equal to 2.9: 1: 0.9: 0.8. In these fractions the photochemical separation of charges could be demonstrated by accumulation of reduced pheophytin (A of 430–440 nm) and by the flash induced formation of P680⁺ (A at 820 nm). The relatively slow relaxation kinetics of the latter signal (t_1/2 1 ms) may suggest that in a substantial fraction of the RCs Q_A remains bound to the complex.Abbreviations Car -carotene - Chl a chlorophyll a - CP43, CP47 chlorophyll-proteins, with R_m 43 and 47 kDa - DBMIB dibromothymoquinone,2,5-dibromo-3-methyl-6-isopropyl-1,4-benzoquinone - DM -dodecyl-d-maltoside - HPLC high-performance liquid chromatography - OG n-octyl--d-glucopyranoside - IMAC immobilied metal affinity chromatography - Pheo a pheophytin a - PQ-9 plastoquinone-9 - P680 primary electron donor in PS II - PS II RC Photosystem II reaction centre - Q_A primary electron acceptor in PS II - SB-12 N-dodecyl-N,N-dimethyl-3-amino-1-propanesulphonate, (sulphobetain 12)     

Influence of temperature on Photosystem II electron transfer reactions

The influence of temperature on the rate of reduction of P-680⁺, the primary donor of Photosystem II, has been studied in the range 5–294 K, in chloroplasts and subchloroplasts particles. P-680 was oxidized by a short laser flash. Its oxidation state was followed by the absorption level at 820 nm, and its reduction attributed to two mechanisms: electron donation from electron donor D₁ and electron return from the primary plastoquinone (back-reaction).Between 294 and approx. 200 K, the rate of the back-reaction, on a logarithmic scale, is a linear function of the reciprocal of the absolute temperature, corresponding to an activation energy between 3.3 and 3.7 kcal · mol^?1, in all of the materials examined (chloroplasts treated at low pH or with Tris; particles prepared with digitonin). Between approx. 200 K and 5 K the rate of the back-reaction is temperature independent, with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 1.6}\text{ms}$. In untreated chloroplasts we measured a $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$ of 1.7 ms for the back-reaction at 77 and 5 K.The rate of electron donation from the donor D₁ has been measured in darkadapted Tris-treated chloroplasts, in the range 294–260 K. This rate is strongly affected by temperature. An activation energy of 11 kcal · mol^?1 was determined for this reaction.In subchloroplast particles prepared with Triton X-100 the signals due to P-680 were contaminated by absorption changes due to the triplet state of chlorophyll a. This triplet state has been examined with pure chlorophyll a in Triton X-100. An Arrhenius plot of its rate of decay shows a temperature-dependent region (292–220 K) with an activation energy of 9 kcal · mol^?1, and a temperature-independent region (below 200 K) with $\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 1.1}\text{ms}$.     

The functional sites of chlorophylls in D1 and D2 subunits of Photosystem II identified by pulsed EPR

The functional site of Chl_Z, an auxiliary electron donor to P680⁺, was determined by pulsed ELDOR applied to a radical pair of Y_D^• and Chlz⁺ in oriented PS II membranes from spinach. The radical-radical distance was determined to be 29.5 Å and its direction was 50° from the membrane normal, indicating that a chlorophyll on the D2 protein is responsible for the EPR Chlz⁺ signal. Spin polarized ESEEM (Electronin Spin Echo Envelop Modulation) of a ³Chl and Q_A⁻ radical pair induced by a laser flash was observed in reaction center D1D2Cytb₅₅₉ complex, in which Q_A was functionally reconstituted with DBMIB and reduced chemically. Q_A⁻ESEEM showed a characteristic oscillating time profile due to dipolar coupling with ³Chl. By fitting with the dipolar interaction parameters, the distance between ³Chl and Q_A⁻ was determined to be 25.9 Å, indicating that the accessory chlorophyll on the D1 protein is responsible for the ³Chl signal.     

The donor side of Photosystem II as the copper-inhibitory binding site

We have measured, under Cu (II) toxicity conditions, the oxygen-evolving capacity of spinach PS II particles in the Hill reactions H₂OSiMo (in the presence and absence of DCMU) and H₂OPPBQ, as well as the fluorescence induction curve of Tris-washed spinach PS II particles. Cu (II) inhibits both Hill reactions and, in the first case, the DCMU-insensitive H₂O SiMo activity. In addition, the variable fluorescence is lowered by Cu (II). We have interpreted our results in terms of a donor side inhibition close to the reaction center. The same polarographic and fluorescence measurements carried out at different pHs indicate that Cu (II) could bind to amino acid residues that can be protonated and deprotonated. In order to reverse the Cu (II) inhibition by a posterior EDTA treatment, in experiments of preincubation of PS II particles with Cu (II) in light we have demonstrated that light is essential for the damage due to Cu (II) and that this furthermore is irreversible.Abbreviations DCMU 3-(3,4-dichlorophenyl)-1, 1-dimethyl urea - DCIP 2,6-dichlorophenolindophenol - DPC 1,5-diphenilcarbazide - F_o initial non-variable fluorescence - F_I intermediate fluorescence yield - F_m maximum fluorescence yield - F_v variable fluorescence yield - Mes 2,-(N-morpholino)ethanosulfonic acid - OEC oxygen-evolving complex - P680 Primary electron donor chlorophyll - Pheo pheophytin - PPBQ phenyl-p-benzo-quinone - PS II Photosystem II - SiMo Silicomolybdate - Q_B secondary quinone acceptor - Q_A primary quinone aceptor - Tris N-tris(hydroxymethyl)amino ethane - Tyr_z electron carrier functioning between P680 and the Mn cluster This article is dedicated to Prof. Dr. Harmut Lichtenthaler on the occasion of his 60th birthday.     

Light-harvesting chlorophyll a-b complex requirement for regulation of Photosystem II photochemistry by non-photochemical quenching

Recently, it has been suggested (Horton et al. 1992) that aggregation of the light-harvesting a-b complex (LHC II) in vitro reflects the processes which occur in vivo during fluorescence induction and related to the major non-photochemical quenching (qE). Therefore the requirement of this chlorophyll a-b containing protein complex to produce qN was investigated by comparison of two barley mutants either lacking (chlorina f2) or depressed (chlorina¹⁰⁴) in LHC II to the wild-type and pea leaves submitted to intermittent light (IL) and during their greening in continuous light. It was observed that qN was photoinduced in the absence of LHC II, i.e. in IL grown pea leaves and the barley mutants. Nevertheless, in these leaves qN had no (IL, peas) or little (barley mutants) inhibitory effect on the photochemical efficiency of Q_A reduction measured by flash dosage response curves of the chlorophyll fluorescence yield increase induced by a single turn-over flash During greening in continuous light of IL pea leaves, an inhibitory effect on Q_A photoreduction associated to qN developed as Photosystem II antenna size increased with LHC II synthesis. Utilizing data from the literature on connectivity between PS II units versus antenna size, the following hypothesis is put forward to explain the results summarized above. qN can occur in the core antenna or Reaction Center of a fraction of PS II units and these units will not exhibit variable fluorescence. Other PS II units are quenched indirectly through PS II-PS II exciton transfer which develops as the proportion of connected PS II units increases through LHC II synthesis.     

The effect of outer antenna complexes on the photochemical trapping rate in barley thylakoid Photosystem II

We have investigated the previous suggestions in the literature that the outer antenna of Photosystem II of barley does not influence the effective photosystem primary photochemical trapping rate. It is shown by steady state fluorescence measurements at the F₀ fluorescence level of wild type and the chlorina f2 mutant, using the chlorophyll b fluorescence as a marker, that the outer antenna is thermally equilibrated with the core pigments, at room temperature, under conditions of photochemical trapping. This is in contrast with the conclusions of the earlier studies in which it was suggested that energy was transferred rapidly and irreversibly from the outer antenna to the Photosystem II core. Furthermore, the effective trapping time, determined by single photon counting, time-resolved measurements, was shown to increase from 0.17±0.017 ns in the chlorina Photosystem II core to a value within the range 0.42±0.036-0.47±0.044 ns for the wild-type Photosystem II with the outer antenna system. This 2.5-2.8-fold increase in the effective trapping time is, however, significantly less than that expected for a thermalised system. The data can be explained in terms of the outer antenna increasing the primary charge separation rate by about 50%.     

Synthetic quinones influencing herbicide binding and Photosystem II electron transport. The effects of triazine-resistance on quinone binding properties in thylakoid membranes

We have analyzed the binding of synthetic quinones and herbicides which inhibit electron transport at the acceptor side of Photosystem II (PS II) of the photosynthetic electron-transport chain in thylakoid membranes. These data show that quinones and PS II-directed herbicides compete for binding to a common binding environment within a PS II region which functions as the Q⁻ / PQ oxidoreductase. We observed that (1) synthetic quinones cause a parallel inhibition of electron transport and [¹⁴C]herbicide displacement, and (2) herbicide binding is affected both by the fully oxidized and fully reduced form of a quinone. Quinone function and inhibitor binding were also investigated in thylakoids isolated from triazine-resistant weed biotypes. We conclude the following. (1) The affinity of the secondary accepting quinone, B, is decreased in resistant thylakoids. (2) The observation that the equilibrium concentration of reduced Q after transferring one electron to the acceptor side of PS II is increased in resistant as compared to susceptible chloroplasts may be explained both by a decrease in the affinity of PQ for the herbicide / quinone binding environment, and by a decrease of the midpont redox potential of the B / B⁻ couple. (3) The binding environment regulating quinone and herbicide affinity may be divided roughly into two domains; we suggest that the domain regulating quinone head-group binding is little changed in resistant membranes, whereas the domain-regulating quinone side-group binding (and atrazine) is altered. This results in increased inhibitory activity of tetrachloro-p-benzoquinone and phenolic herbicides, which are hypothesized to utilize the quinone head-group domain. The two domains appear to be spatially overlapping because efficient atrazine displacement by tetrachloro-p-benzoquinone is observed.