Detection of oxygen-evolving Photosystem II centers inactive in plastoquinone reduction

Quite different estimates of the number of Photosystem II centers present in thylakoid membranes are obtained depending on the technique used in making the determination. By using brief saturating light flashes and measuring the electron transport per flash, we have obtained two values for the number of functional centers. When the electrons produced reduce the intersystem plastoquinone pool, there are about 1.7 mmol of active Photosystem II centers per mol chlorophyll, whereas there are at least 3 mmol of active centers per mol chlorophyll when certain halogenated benzoquinones are being reduced. There are also at least 3 mmol of terbutryn binding sites per mol of chlorophyll when this tightly binding herbicide is employed as a specific inhibitor of Photosystem II. Thus only about 60% of the membrane's total complement of Photosystem II centers are able to transfer electrons to Photosystem I at appreciable rates. Many functional assays requiring significant rates of turnover sample only this more active pool, whereas herbicide-binding studies and measurements of changes in the Photosystem II electron donor Z and electron acceptor Q_A performed by other investigators reveal, in addition, a large population of Photosystem II reaction centers that normally have negligible turnover numbers. However, these normally inactive centers readily transfer electrons to the halogenated benzoquinones and are then counted among the active centers. Therefore, it can be concluded that all of herbicide-binding sites represent centers with operative water-oxidizing reactions. It can also be concluded that there are few, if any, centers capable of binding more than a single herbicide molecule.     

Cyclic electron flow around Photosystem II in vivo

The oxygen flash yield (Y_O2) and photochemical yield of PS II (_{PS II}) were simultaneously detected in intact Chlorella cells on a bare platinum oxygen rate electrode. The two yields were measured as a function of background irradiance in the steady-state and following a transition from light to darkness. During steady-state illumination at moderate irradiance levels, Y_O2 and _{PS II} followed each other, suggesting a close coupling between the oxidation of water and Q_A reduction (Falkowski et al. (1988) Biochim. Biophys. Acta 933: 432–443). Following a light-to-dark transition, however, the relationship between Q_A reduction and the fraction of PS II reaction centers capable of evolving O₂ became temporarily uncoupled. _{PS II} recovered to the preillumination levels within 5–10 s, while the Y_O2 required up to 60 s to recover under aerobic conditions. The recovery of Y_O2 was independent of the redox state of Q_A, but was accompanied by a 30% increase in the functional absorption cross-section of PS II (_{PS II}). The hysteresis between Y_O2 and the reduction of Q_A during the light-to-dark transition was dependent upon the reduction level of the plastoquinone pool and does not appear to be due to a direct radiative charge back-reaction, but rather is a consequence of a transient cyclic electron flow around PS II. The cycle is engaged in vivo only when the plastoquinone pool is reduced. Hence, the plastoquinone pool can act as a clutch that disconnects the oxygen evolution from photochemical charge separation in PS II.Abbreviations ADRY acceleration of the deactivation reactions of the water-splitting enzyme (agents) - Chl chlorophyll - cyt cytochrome - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - F_O minimum fluorescence yield in the dark-adapted state - F_I minimum fluorescence yield under ambient irradiance or during transition from the light-adapted state - F_M maximum fluorescence yield in the dark-adapted state - F_M maximum fluorescence yield under ambient irradiance or during transition from light-adapted state - F_V, F_V variable fluorescence (F_V=F_M–F_O ; F_V=F_M–F_I) - FRR fast repetition rate (fluorometer) - _{PS II} quantum yield of Q_A reduction (_{PS II}=(F_M – F_O)/F_M or _{PS II})=(F_M= – F_I=)/F_M=) - LHCII Chl a/b light harvesting complexes of Photosystem II - OEC oxygen evolving complex of PS II - P680 reaction center chlorophyll of PS II - PQ plastoquinone - POH₂ plastoquinol - PS I Photosystem I - PS II Photosystem II - RC II reaction centers of Photosystem II - PS II the effective absorption cross-section of PHotosystem II - TL thermoluminescence - Y_O2 oxygen flash yield The US Government right to retain a non-exclusive, royalty free licence in and to any copyright is acknowledged.     

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.     

Investigation of the plastoquinone pool size and fluorescence quenching in thylakoid membranes and Photosystem II (PS II) membrane fragments

The efficiency of oxidized endogenous plastoquinone-9 (PQ-9) as a non-photochemical quencher of chlorophyll fluorescence has been analyzed in spinach thylakoids and PS II membrane fragments isolated by Triton X-100 fractionation of grana stacks. The following results were obtained: (a) After subjection of PS II membrane fragments to ultrasonic treatment in the presence of PQ-9, the area over the induction curve of chlorophyll fluorescence owing to actinic cw light increases linearly with the PQ-9/PS II ratio in the reconstitution assay medium; (b) the difference of the maximum fluorescence levels, F_max, of the induction curves, measured in the absence and presence of DCMU, is much more pronounced in PS II membrane fragments than in thylakoids; (c) the ratio F_max(-DCMU)/F_max(+DCMU) increases linearly with the content of oxidized PQ-9 that is varied in the thylakoids by reoxidation of the pool after preillumination and in PS II membrane fragments by the PQ-9/PS II ratio in the reconstitution assay; (d) the reconstitution procedure leads to tight binding of PQ-9 to PS II membrane fragments, and PQ-9 cannot be replaced by other quinones; (e) the fluorescence quenching by oxidized PQ-9 persists at low temperatures, and (f) oxidized PQ-9 preferentially affects the F695 of the fluorescence emission spectrum at 77 K. Based on the results of this study the oxidized PQ-9 is inferred to act as a non-photochemical quencher via a static mechanism. Possible implications for the nature of the quenching complex are discussed. This revised version was published online in June 2006 with corrections to the Cover Date.     

Electron transfer in the water-oxidizing complex of Photosystem II

An overview is presented of secondary electron transfer at the electron donor side of Photosystem II, at which ultimately two water molecules are oxidized to molecular oxygen, and the central role of manganese in catalyzing this process is discussed. A powerful technique for the analysis of manganese redox changes in the water-oxidizing mechanism is the measurement of ultraviolet absorbance changes, induced by single-turnover light flashes on dark-adapted PS II preparations. Various interpretations of these ultraviolet absorbance changes have been proposed. Here it is shown that these changes are due to a single spectral component, which presumably is caused by the oxidation of Mn(III) to Mn(IV), and which oscillates with a sequence +1, +1, +1, –3 during the so-called S₀ S₁ S₂ S₃ S₀ redox transitions of the oxygen-evolving complex. This interpretation seems to be consistent with the results obtained with other techniques, such as those on the multiline EPR signal, the intervalence Mn(III)-Mn(IV) transition in the infrared, and EXAFS studies. The dark distribution of the S states and its modification by high pH and by the addition of low concentrations of certain water analogues are discussed. Finally, the patterns of proton release and of electrochromic absorbance changes, possibly reflecting the change of charge in the oxygen-evolving system, are discussed. It is concluded that nonstoichiometric patterns must be considered, and that the net electrical charge of the system probably is the highest in state S₂ and the lowest in state S₁.     

Interaction of electron acceptors with thylakoids from halophytic and non-halophytic species

Thylakoid membranes isolated from halophytic species showed differences in their interactions with ionic and lipophilic electron acceptors when compared to thylakoids from non-halophytes. FeCN was considerably less efficient as electron acceptor with halophyte thylakoids, supporting much lower rates of O₂ evolution and having a lower affinity. FeCN accepted electrons at a different, DMMIB insensitive, site with these thylakoids. 1,4-Benzo-quinones with less positive midpoint potentials were less effective in accepting electrons from halophyte thylakoids compared to nonhalophyte thylakoids, also reflected in lower rates of O₂ evolution and lower affinity. Considering the lipolphilic nature and the fact that there was no apparent change in the site donating electrons to the quinones, an alteration in the midpoint potential of this site by about +100mV is postulated for the halophyte thylakoids.Abbreviations AMPD 2-amino-2-methyl-1,3-propanediol - Cyt b₆/f cytochrome b₆/f complex - DBMIB 2,5-dibromo-6-isopropyl-3-methyl-1,4-benzoquinone - DCBQ 2,6-dichloro-1,4-benzoquinone - DCIP 2,6-dichlorophenol-indolphenol - DMBQ 2,5-dimethyl-1,4-benzoquinone - E_m7 midpoint redox potential at pH 7.0, FeCN-K₃Fe(CN)₆ - HNQ 5-hydroxy-1,4-naphthoquinone - MV methylviologen - NQ 1,4-naphthoquinone - PBQ phenyl-1,4-benzoquinone - PC plastocyanin - PQ plastoquinone     

Redox titration of electron acceptor Q and the plastoquinone pool in Photosystem II

The primary photochemical quencher Q and the secondary electron acceptor pool in Photosystem II have been titrated. We used particles of Scenedesmus mutant No. 8 that lack System I and allowed the system to equilibrate with external redox mediators in darkness prior to measurement of the fluorescence rise curve.The titration of Q, as indicated by the dark level of F_i, occurs in two discrete steps. The high-potential component (Q_h) has a midpoint potential of +68 mV (pH 7.2) and accounts for ～67% of Q. The pH sensitivity of the midpoint potential is ?60 mV, indicating the involvement of 1 $\text{H}{}^{\mathrm{+}}\text{e}$. The low-potential component (Q₁) accounts for the remaining 33% of Q and shows a midpoint potential near?300 mV (pH 7.2).The plastoquinone pool, assayed as the half-time of the fluorescence rise curve, titrates as a single component with a midpoint potential 30–40 mV more oxidizing than that of Q_h, i.e., at 106 mV (pH 7.2). The E_m shows a pH sensitivity of ?60 mV/pH unit, indicating the involvement of 1 $\text{H}{}^{\mathrm{+}}\text{e}$. The observation that all 12–14 electron equivalents in the pool titrate as a single component indicates that the heterogeneity otherwise observed in the secondary acceptor system is a kinetic rather than a thermodynamic property.Illumination causes peculiar, and as yet unclarified, changes of both Q and the secondary pool under anaerobic conditions that are reversed by oxygen.     

The deactivation of Photosystem II in Chlorella as a second-order process

The kinetics of deactivation of the S₃ state in Chlorella have been observed under a variety of conditions. The S₃ state appears to decline in a dark period coming after a sequence of 30 saturating flashes in a second-order reaction, the rate constant of which is 0.132/[S*₃] s⁻¹ and which involves an electron donor, D₁, of concentration 1.25[S*₃] where [S*₃] is the concentration of the S₃ state when the oxygen yield of the light flashes is constant. If a 1 min period of 650 nm illumination is employed after the sequence of flashes, the subsequent S₃ state deactivation kinetics are more complex. There is an initial phase of S₃ state deactivation, accounting for about 35% of the original S₃ state, which is complete in less than 100 ms. The remaining 65% of the S₃ state appears to deactivate in a second-order reaction, the rate constant of which is 1.36/[S*₃] s⁻¹ and which involves an electron donor of initial concentration 0.58[S*₃]. If a 1 min period of 710 nm illumination comes after the 30 flashes, at least 98% of the S₃ state deactivates according to first-order kinetics. It is shown that this can be explained using a second-order model if there is an electron donor present of which the concentration is large compared with [S*₃]. However, S₃ state deactivation observed after 5 min of dark and two saturating flashes can be described neither by a first-order model nor a second-order model. Deactivation of the S₂ state after a 5 min dark period and one saturating flash follows second-order kinetics with a rate constant of 0.2/[S*₃] s⁻¹ and appears to involve an electron donor of initial concentration 1.3[S*₃]. Arguments are presented which tend to rule out the primary electron acceptor to Photosystem II as being any of the electron donors but it appears quite possible that the large plastoquinone pool is involved.     

The inhibitory mechanism of Cu(II) on the Photosystem II electron transport from higher plants

In a previous paper, we reported that Cu(II) inhibited the photosynthetic electron transfer at the level of the pheophytin-Q_A-Fe domain of the Photosystem II reaction center. In this paper we characterize the underlying mechanism of Cu(II) inhibition. Cu(II)-inhibition effect was more sensitive with high pH values. Double-reciprocal plot of the inhibition of oxygen evolution by Cu(II) is shown and its corresponding inhibition constant, K_i, was calculated. Inhibition by Cu(II) was non-competitive with respect to 2,6-dichlorobenzoquinone and 3-(3,4-dichlorophenyl)-1,1-dimethylurea and competitive with respect to protons. The non-competitive inhibition indicates that the Cu(II)-binding site is different from that of the 2,6-dichlorobenzoquinone electron acceptor and 3-(3,4-dichlorophenyl)-1,1-dimethylurea sites, the Q_B niche. On the other hand, the competitive inhibition with respect to protons may indicate that Cu(II) interacts with an essential amino acid group(s) that can be protonated or deprotonated in the inhibitory-binding site.Abbreviations BSA bovine seroalbumin - Chl chlorophyll - DCBQ 2,6-dichlorobenzoquinone - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - MES 2-(N-morpholino)-ethanesulphonic acid - Pheo pheophytin - Q_A primary quinone acceptor - Q_B secondary quinone acceptor - PS Photosystem - RC reaction center - Tricine N-[Tris(hydroxymethyl)-methyl]-glycine     

On the rates of cyclic electron transport around Photosystem II in the presence of donor side limitation

Photosystem II cyclic electron transport was investigated at low pH in spinach thylakoids and PS II preparations from the cyanobacteriumPhormidium laminosum. Variable fluorescence (F_v) quenching at a very low light intensity was examined as an indicator of cyclic electron flow. A progressive quenching of F_v was observed as the pH was lowered; however, this was shown to be mainly due to an inhibition of oxygen evolution. Cyclic electron flow in the uninhibited centres was estimated to occur at a rate comparable to or smaller than 1 mole O₂ mg Chl^–1 h^–1 in the pH range 5.0 to 7.8.The quantum yeeld of oxygen production is known to decrease at low pH and has been taken to indicate cyclic electron flow (Crofts and Horton (1991) Biochim Biophys Acta 1058: 187–193). However, a direct all-or-none inhibition of oxygen production at low pH has also been reported (Meyer et al. (1989) Biochim Biophys Acta 974: 36–43). We have analysed the effects of light intensity on the rates of oxygen evolution in order to calculate _U, the quantum yield of open and uninhibited centres. _U was found to be constant over a broad pH range, and by using ferricyanide and phenyl-p-benzoquinone as electron acceptors the maximum possible rate of cyclic electron transport was equivalent to no more than 1 mole O₂ mg Chl^–1 h^–1. The rate was no greater when the acceptor was adjusted to provide the most favourable conditions for cyclic flow.     

Mn2+ reduces Yz + in manganese-depleted Photosystem II preparations

Manganese in the oxygen-evolving complex is a physiological electron donor to Photosystem II. PS II depleted of manganese may oxidize exogenous reductants including benzidine and Mn²⁺. Using flash photolysis with electron spin resonance detection, we examined the room-temperature reaction kinetics of these reductants with Y_z ⁺, the tyrosine radical formed in PS II membranes under illumination. Kinetics were measured with membranes that did or did not contain the 33 kDa extrinsic polypeptide of PS II, whose presence had no effect on the reaction kinetics with either reductant. The rate of Y_z ⁺ reduction by benzidine was a linear function of benzidine concentration. The rate of Y_z ⁺ reduction by Mn²⁺ at pH 6 increased linearly at low Mn²⁺ concentrations and reached a maximum at the Mn²⁺ concentrations equal to several times the reaction center concentration. The rate was inhibited by K⁺, Ca²⁺ and Mg²⁺. These data are described by a model in which negative charge on the membrane causes a local increase in the cation concentration. The rate of Y_z ⁺ reduction at pH 7.5 was biphasic with a fast 400 s phase that suggests binding of Mn²⁺ near Y_z ⁺ at a site that may be one of the native manganese binding sites.Abbreviations PS II Photosystem II - Y_D tyrosine residue in Photosystem II that gives rise to the stable Signal II EPR spectrum - Y_z tyrosine residue in Photosystem II that mediates electron transfer between the reaction center chlorophyll and the site of water oxidation - ESR electron spin resonance - DPC diphenylcarbazide - DCIP dichlorophenolindophenol     

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.     

Improvement of four sigma analysis for the investigation of oxygen evolution by Photosystem II

We present here an improvement to the analysis of oxygen evolution with four sigma coefficients (4-S) by computing z, the sum of the S-state probabilities, which was introduced earlier (Delrieu and Rosengard 1987, Biochim Biophys Acta 892: 163–171). We demonstrate that z is equal to the ratio of two consecutive Mean Y (the estimation of the steady state oxygen production based on local properties) found by three sigma analysis. The quantity z is useful for computing double-hits, and for showing the inactivation/activation processes of PS II complexes. Three sigma analysis assumes z=1 exactly; since this is not verified, it is argued that four sigma analysis is closer to the real workings of the water oxidizing complex. Oxygen evolution can then be interpreted in the frame of a modified Kok's model where the sum of the probabilities equals z. We therefore suggest that the closer fitting of four sigma analysis to oxygen production data is not simply due to an extra, unnecessary variable, but to the fact that PS II complexes can be inactivated and reactivated under flashing light. Finally, in order to facilitate the use of four sigma analysis, a computer program is made available upon request.     

Nitrogen ligation to the manganese cluster of Photosystem II in the absence of the extrinsic proteins and as a function of pH

Three extrinsic proteins (PsbO, PsbP and PsbQ), with apparent molecular weights of 33, 23 and 17 kDa, bind to the lumenal side of Photosystem II (PS II) and stabilize the manganese, calcium and chloride cofactors of the oxygen evolving complex (OEC). The effect of these proteins on the structure of the tetramanganese cluster, especially their possible involvement in manganese ligation, is investigated in this study by measuring the reported histidine-manganese coupling [Tang et al. (1994) Proc Natl Acad Sci USA 91: 704–708] of PS II membranes depleted of none, two or three of these proteins using ESEEM (electron spin echo envelope modulation) spectroscopy. The results show that neither of the three proteins influence the histidine ligation of manganese. From this, the conserved histidine of the 23 kDa protein can be ruled out as a manganese ligand. Whereas the 33 and 17 kDa proteins lack conserved histidines, the existence of a 33 kDa protein-derived carboxylate ligand has been posited; our results show no evidence for a change of the manganese co-ordination upon removal of this protein. Studies of the pH-dependence of the histidine–manganese coupling show that the histidine ligation is present in PS II centers showing the S₂ multiline EPR signal in the pH-range 4.2–9.5. This revised version was published online in June 2006 with corrections to the Cover Date.     

Intactness of the oxygen-evolving system in thylakoids and Photosystem II particles

Photosystem II activity of oxygen-evolving membranes can be quantified by their capacity to do charge separation or their capacity to transport electrons. In this study using flash excitation of saturating intensity, charge separation is measured by absorption changes in the ultraviolet region of the spectra associated with primary-quinone reduction, and electron transport is measured by oxygen flash yield. These methods are applied to thylakoids and three different types of Photosystem II particles. In thylakoids electron-transport activity is 75–85% of charge separation activity. In Photosystem II particles this percentage is 60–70%, except for the BBY type (Berthold, D.A., Babcock, G.T. and Yocum, C.F. (1981) FEBS Lett. 135, 231–234), in which it is only 29%. These estimates of non-functional oxygen-evolving centers agree within experimental error, except for the BBY particle, with the quantum requirement for oxygen evolution measured under light-limited conditions. These reaction centers that are non-functional in oxygen evolution occur during sample preparation and are not a result of inhibition by ferricyanide or quinone acceptor systems. In thylakoids on the first flash, absorption changes at 325 nm do not show significant contributions from oxygen evolution S-state transitions. In the presence of ferricyanide the absorption change at 325 nm does have a significant contribution from Q₄₀₀ in thylakoids, but considerably less in Photosystem II particles.     

Effects of bicarbonate depletion on secondary acceptors of Photosystem II

In thylakoid membranes incubated in the dark with ferricyanide, an auxiliary acceptor (Q400) associated with Photosystem II becomes oxidized. It has been reported that, based on oxygen flash-yield data, electron flow to Q400 did not occur in ‘bicarbonate-depleted’ (formate-pretreated) samples. Contrary to this earlier report, we find, based on oxygen flash-yield data and chlorophyll a fluorescence-transient measurements, that Q400 is active as an electron acceptor in formate-pretreated samples. It is concluded that the effect of formate pretreatment is on the flow of electrons between Q, B and the plastoquinone pool and not the flow to Q400. We also believe that another auxiliary acceptor of Photosystem II exists under conditions of formate pretreatment and pH larger than 7.0. This belief is based on increased double advancement in the oxygen flash-yield pattern and increased area above the chlorophyll a fluorescence-rise curve. The double advancement in the oxygen pattern shows a second-order dependence on flash intensity. These effects are eliminated by bicarbonate addition or shifts to lower values of pH such as 6.8. This new acceptor is believed to be different from Q400.     

Mode of action of Photosystem II herbicides studied by thermoluminescence

The mode of action of chemically different herbicides (ureas, pyridazinones, phenylcarbamates, triazines, hydroxyquinolines, hydroxybenzonitriles and dinitrophenols) on photosynthetic electron transport was investigated by measurements of oxygen evolution and thermoluminescence. Depending on the particular herbicide used the thermoluminescence band related to Q (the primary acceptor of Photosystem II) appears at +5, 0 or −14°C. It was shown that these three different peak positions can be ascribed to various redox states of Q, the shifts being due to the binding of herbicides to the chloroplast membrane. Both displacement experiments and additive inhibition of herbicide pairs measured by thermoluminescence and oxygen evolution suggested that the sites of action of these herbicides are on the same protein. However, herbicide treatment of trypsinized chloroplasts showed that there were three different binding sites on the same protein, in agreement with the classification of herbicides into three groups based on thermoluminescence measurements. Our results suggest that the primary and secondary acceptors of Photosystem II (Q and B, respectively) are in close proximity and form a common complex with the herbicide-binding protein within the chloroplast membrane.