A new EPR signal attributed to the primary plastosemiquinone acceptor in Photosystem II

A study of signals, light-induced at 77 K in O₂-evolving Photosystem II (PS II) membranes showed that the EPR signal that has been attributed to the semiquinone-iron form of the primary quinone acceptor, Q^?_AFe, at g = 1.82 was usually accompanied by a broad signal at g = 1.90. In some preparations, the usual g = 1.82 signal was almost completely absent, while the intensity of the g = 1.90 signal was significantly increased. The g = 1.90 signal is attributed to a second EPR form of the primary semiquinone-iron acceptor of PS II on the basis of the following evidence. (1) The signal is chemically and photochemically induced under the same conditions as the usual g = 1.82 signal. (2) The extent of the signal induced by the addition of chemical reducing agents is the same as that photochemically induced by illumination at 77 K. (3) When the g = 1.82 signal is absent and instead the g = 1.90 signal is present, illumination at 200 K of a sample containing a reducing agent results in formation of the characteristic split pheophytin^? signal, which is thought to arise from an interaction between the photoreduced pheophytin acceptor and the semiquinone-iron complex. (4) Both the g = 1.82 and g = 1.90 signals disappear when illumination is given at room temperature in the presence of a reducing agent. This is thought to be due to a reduction of the semiquinone to the nonparamagnetic quinol form. (5) Both the g = 1.90 and g = 1.82 signals are affected by herbicides which block electron transfer between the primary and secondary quinone acceptors. It was found that increasing the pH results in an increase of the g = 1.90 form, while lowering the pH favours the g = 1.82 form. The change from the g = 1.82 form to the g = 1.90 form is accompanied by a splitting change in the split pheophytin^? signal from approx. 42 to approx. 50 G. Results using chloroplasts suggest that the g = 1.90 signal could represent the form present in vivo.     

Comparative EPR and thermoluminescence study of anoxic photoinhibition in Photosystem II particles

Photosystem II particles were exposed to 800 W m^–2 white light at 20 °C under anoxic conditions. The F_o level of fluorescence was considerably enhanced indicating formation of stable-reduced forms of the primary quinone electron acceptor, Q_A. The F_m level of fluorescence declined only a little. The g=1.9 and g=1.82 EPR forms characteristic of the bicarbonate-bound and bicarbonate-depleted semiquinone-iron complex, Q_A ^–Fe²⁺, respectively, exhibited differential sensitivity against photoinhibition. The large g=1.9 signal was rapidly diminished but the small g=1.82 signal decreased more slowly. The S₂-state multiline signal, the oxygen evolution and photooxidation of the high potential form of cytochrome b-559 were inhibited approximately with the same kinetics as the g=1.9 signal. The low potential form of oxidized cytochrome b-559 and Signal II_slow arising from Tyr_D ⁺ decreased considerably slower than the g=1.9 semiquinone-iron signal. The high potential form of oxidized cytochrome b-559 was diminished faster than the low potential form. Photoinhibition of the g=1.9 and g=1.82 forms of Q_A was accompanied with the appearance and gradual saturation of the spin-polarized triplet signal of P 680. The amplitude of the radical signal from photoreducible pheophytin remained constant during the 3 hour illumination period. In the thermoluminescence glow curves of particles the Q band (S₂Q_A ^– charge recombination) was almost completely abolished. To the contrary, the C band (Tyr_D ⁺Q_A ^– charge recombination) increased a little upon illumination. The EPR and thermoluminescence observations suggest that the Photosystem II reaction centers can be classified into two groups with different susceptibility against photoinhibition.Abbreviations C band thermoluminescence band associated with Tyr-D⁺Q _a ^– charge recombination - Chl chlorophyll - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - EPR electron paramagnetic resonance - F_o initial fluorescence - F_m maximum fluorescence - Q band thermoluminescence band originating from S₂Q _a -charge recombination - Q _a the primary quinone electron acceptor of PS II - P 680 the primary electron donor chlorophyll of PS II - S₂ oxidation state of the water-splitting system - Phe pheophytin - TL thermoluminescence - Tyr _d redox active tyrosine-160 of the D₂ protein     

Photoreductant-induced oxidation of Fe2+ in the electron-acceptor complex of Photosystem II

The ferrous ion associated with the electron acceptors in Photosystem II can be oxidized by the unstable semiquinone form of certain high-potential quinones (phenyl-p-benzoquinone, dimethylbenzoquinone and benzoquinone) which are used as electron acceptors. In a flash sequence, alternating oxidation of the iron by the photoreduced semiquinone on odd-numbered flashes is followed by photoreduction of the iron on even-numbered flashes. These reactions are detected by monitoring EPR signals arising from Fe³⁺. The oxidation of the iron can also occur in the frozen state (−30°C) indicating that the high-potential quinone can occupy the Q_B site. The reaction also takes place when the exogenous quinone is added in the dark to samples in which Q_B is already in the semiquinone form. The inhibitors of electron transfer between Q_A⁻ and Q_B, DCMU and sodium formate, block the photoreductant-induced iron oxidation. It is suggested that the iron oxidation takes place through the Q_B site. This unexpected photochemistry occurs under experimental conditions routinely used in studies of Photosystem II. Some previously reported phenomena can be reinterpreted on the basis of these new data.     

Electrogenic reduction of the secondary quinone acceptor in chromatophores of Rhodospirillum rubrum: Rapid kinetics measurements

Electron transfer Q_A → Q_B has been reconstituted with added Q-10 in Rhodospirillum rubrum chromatophores associated with a phospholipid-impregnated collodion film. Rapid kinetics measurements of laser flash-induced ΔΨ generated in the chromatophores show that whereas electron transfer from Q_a⁻ to Q_B upon the first flash is not electrogenic in dark-adapted chromatophores, reduction of Q⁻_B to Q_bh₂ induced by the second flash gives rise to an electrogenic phase with τ = 250 μs at pH 7.5 which contributes about 10% to the total ΔΨ generated upon the flash. The electrogenic phase is ascribed to vectorial protonation of Q²⁻_B.     

Oxidation-reduction properties of the electron acceptors of Photosystem II. II. Redox titration at various pH values of the flash-induced formation of C550 in Chlamydomonas Photosystem II particles lacking the secondary quinone electron acceptor

Redox titrations of the flash-induced formation of C550 (a linear indicator of Q^?) were performed between pH 5.9 and 8.3 in Chlamydomonas Photosystem II particles lacking the secondary electron acceptor, B. One-third of the reaction centers show a pH-dependent midpoint potential (E_m,7.5) = ? 30 mV) for redox couple $\text{Q}\text{Q}{}^{\mathrm{?}}$, which varies by ?60 mV/pH unit. Two-thirds of the centers show a pH-independent midpoint potential (E_mm = + 10 mV) for this couple. The elevated pH-independent E_m suggests that in the latter centers the environment of Q has been modified such as to stabilize the semiquinone anion, Q^?. The midpoint potentials of the centers having a pH-dependent E_m are within 20 mV of those observed in chloroplasts having a secondary electron acceptor. It appears therefore that the secondary electron acceptor exerts little influence on the E_m of $\text{Q}\text{Q}{}^{\mathrm{?}}$. An EPR signal at g 1.82 has recently been attributed to a semiquinone-iron complex which comprises Q^?. The similar redox behavior reported here for C550 and reported by others (Evans, M.C.W., Nugent, J.H.A., Tilling, L.A. and Atkinson, Y.E. (1982) FEBS Lett. 145, 176–178) for the g 1.82 signal in similar Photosystem II particles confirm the assignment of this EPR signal to Q^?. At below ?200 mV, illumination of the Photosystem II particles produces an accumulation of reduced pheophytin (Ph^?). At ?420 mV Ph^? appears with a quantum yield of 0.006–0.01 which in this material implies a lifetime of 30–100 ns for the radical pair P-680⁺Ph^?.     

Orientation of the primary quinone of bacterial photosynthetic reaction centers contined in chromatophore and reconstituted membranes

The orientation of the reaction center bacteriochlorophyll dimer, (BChl)₂, and primary quinone, Q_I, has been studied by EPR in chromatophores of Rhodopseudomonas sphaeroides R26 and Chromatium vinosum and in the reconstituted membrane multilayers of the isolated Rps. sphaeroides reaction center protein. The similarity in the angular dependence of the (BChl)₂ triplet and Q_I?Fe²⁺ signals in the chromatophore and reconstituted reaction center membrane multilayers indicates that the reaction center is similarly oriented in both native and model membranes. The principle magnetic axes of the (BChl)₂ triplet are found to lie with the x direction approximately parallel to the plane of the membrane surface, and the z and y directions approx. 10–20° away from the plane of the membrane surface and membrane normal, respectively. The Q_I?Fe²⁺ signals are found to have the g 1.82 component positioned perpendicular to the plane of the membrane surface, with an orthogonal low-field transition (at g 1.68 in Rps. Sphaeroides and at g 1.62 in C. vinosum) lying parallel to the plane of the membrane surface. The orientation of Q_I was determined by the angular dependence of this signal in Fe²⁺-depleted reaction center reconstituted membrane multilayers, and it was found to be situated most likely with the plane of the quinone ring perpendicular to the plane of the membrane surface.     

Free-energy change accompanying the reduction of the reaction center secondary quinone in Rhodopseudomonas sphaeroides chromatophores

The standard free-energy change accompanying the electron transfer from Q_A to Q_B was estimated from the intensity of the delayed fluorescence in chromatophores of Rhodopseudomonas sphaeroides. The value of 120 meV (at pH 8) suggests that Q_B⁻ is more stable in the chromatophore membrane than in the isolated reaction center.     

Effects of trypsin upon EPR signals arising from components of the donor side of Photosystem II

EPR signals from components functioning on the electron donor side of Photosystem II (PS II) have been monitored in PS II membranes isolated from spinach chloroplasts after treatment with trypsin at pH 7.5 and pH 6.0. The following information has been obtained. (1) The multiline manganese signal, the g = 4.1 signal and Signal II_slow are lost with trypsin treatment at pH 7.5, but not at pH 6.0. (2) At pH 7.5 the multiline S₂ signal and the g = 4.1 signal are lost with approximately the same dependency on the incubation time with trypsin. At pH 6.0 trypsin treatment is known to block electron transfer between Q_A and Q_B (the first and the second quinone electron acceptors, respectively) allowing only a single turnover to occur. Under these conditions both the g = 4.1 signal and the multiline signal are induced by illumination at 200 K and their amplitudes are almost the same as in untreated samples. These results are interpreted as indicating that the g = 4.1 signal arises from a side path donor or from S₂ itself rather than a carrier functioning between the S states and the reaction center as previously suggested. (3) Cytochrome b-559 is converted to its oxidized low-potential form by trypsin treatment at both values of pH. At pH 6.0 the S-state turnover still occurs indicating that the presence of reduced high-potential cytochrome b-559 is not necessary for this process.     

Electron transfer in reaction centers of Rhodopseudomonas sphaeroides. I. Determination of the charge recombination pathway of D+QAQ−B and free energy and kinetic relations between Q−AQB and QAQ−B

The electron-transfer reactions and thermodynamic equilibria involving the quinone acceptor complex in bacterial reaction centers from R. sphaeroides were investigated. The reactions are described by the scheme: We found that the charge recombination pathway of D⁺Q_AQ^?_B proceeds via the intermediate state D⁺Q^?_AQ_B, the direct pathway contributing less than approx. 5% to the observed recombination rate. The method used to obtain this result was based on a comparison of the kinetics predicted for the indirect pathway (given by the product k_AD-times the fraction of reaction centers in the Q^?_AQ_B state) with the observed recombination rate, k^obs_{D⁺ →D}. The kinetic measurements were used to obtain the pH dependence (6.1 ? pH ? 11.7) of the free energy difference between the states Q^?_AQ_B and Q_AQ^?_B. At low pH (less than 9) Q_AQ^?_B is stabilized relative to Q^?_AQ_B by 67 meV, whereas at high pH Q^?_AQ_B is energetically favored. Both Q^?_A and Q^?_B associate with a proton, with pK values of 9.8 and 11.3, respectively. The stronger interaction of the proton with Q^?_B provides the driving force for the forward electron transfer.     

The Semiquinone-Iron Complex of Photosystem II: Structural Insights from ESR and Theoretical Simulation; Evidence that the Native Ligand to the Non-Heme Iron Is Carbonate

The semiquinone-iron complex of photosystem II was studied using electron spin resonance (ESR) spectroscopy and density functional theory calculations. Two forms of the signal were investigated: 1), the native g ∼ 1.9 form; and 2), the g ∼ 1.84 form, which is well known in purple bacterial reaction centers and occurs in photosystem II when treated with formate. The g ∼ 1.9 form shows low- and high-field edges at g ∼ 3.5 and g < 0.8, respectively, and resembles the g ∼ 1.84 form in terms of shape and width. Both types of ESR signal were simulated using the theoretical approach used previously for the BRC complex, a spin Hamiltonian formalism in which the semiquinone radical magnetically interacts (J ∼ 1 cm⁻¹) with the nearby high-spin Fe²⁺. The two forms of ESR signal differ mainly by an axis rotation of the exchange coupling tensor (J) relative to the zero-field tensor (D) and a small increase in the zero-field parameter D (∼6 cm⁻¹). Density functional theory calculations were conducted on model semiquinone-iron systems to identify the physical nature of these changes. The replacement of formate (or glutamate in the bacterial reaction centers) by bicarbonate did not result in changes in the coupling environment. However, when carbonate (CO₃²⁻) was used instead of bicarbonate, the exchange and zero-field tensors did show changes that matched those obtained from the spectral simulations. This indicates that 1), the doubly charged carbonate ion is responsible for the g ∼ 1.9 form of the semiquinone-iron signal; and 2), carbonate, rather than bicarbonate, is the ligand to the iron.     

EPR studies of the oxygen-evolving enzyme of Photosystem II

The light-induced EPR multiline signal is studied in O₂-evolving PS II membranes. The following results are reported: (1) Its amplitude is shown to oscillate with a period of 4, with respect to the number of flashes given at room temperature (maxima on the first and fifth flashes). (2) Glycerol enhances the signal intensity. This effect is shown to come from changes in relaxation properties rather than an increase in spin concentration. (3) Deactivation experiments clearly indicate an association with the S₂ state of the water-oxidizing enzyme. A signal at g = 4.1 with a linewidth of 360 G is also reported and it is suggested that this arises from an intermediate donor between the S states and the reaction centre. This suggestion is based on the following observations: (1) The g = 4.1 signal is formed by illumination at 200 K and not by flash excitation at room temperature, suggesting that it arises from an intermediate unstable under physiological conditions. (2) The formation of the g = 4.1 signal at 200 K does not occur in the presence of DCMU, indicating that more than one turnover is required for its maximum formation. (3) The g = 4.1 signal decreases in the dark at 220 K probably by recombination with Q^?_AFe. This recombination occurs before the multiline signal decreases, indicating that the g = 4.1 species is less stable than S₂. (4) At short times, the decay of the g = 4.1 signal corresponds with a slight increase in the multiline S₂ signal, suggesting that the loss of the g = 4.1 signal results in the disappearance of a magnetic interaction which diminishes the multiline signal intensity. (5) Tris-washed PS II membranes illuminated at 200 K do not exhibit the signal.     

Thermoluminescence study of charge recombination in Photosystem II at low temperatures. II. Oscillatory properties of the Zv and A thermoluminescence bands in chloroplasts dark-adapted for various time periods

The oscillations of the Z_V and A thermoluminescence bands were investigated in spinach chloroplasts which had been dark-adapted for various time periods and subjected to a series of flashes at +2°C before continuous illumination at various low temperatures. When excited with continuous light below −65°C, the Z_V band exhibited period-4 oscillation, with maxima on preflashes 0, 4 and 8. Above −65°C, the oscillation pattern depended greatly on the dark-adaptation period of the chloroplasts. In preilluminated samples (15 s light followed by 3 min dark), when the Q_B pool is half oxidized, the oscillation of the thermoluminescence intensity measured at −50°C was similar to that observed below −65°C. However, after the thorough dark-adaptation of the chloroplasts (6 h), when the major fraction of the Q_B pool is assumed to be oxidized, a binary oscillation appeared in the oscillation pattern, with maxima at odd flash numbers. Below −65°C, period-2 oscillation of the Z_V band could not be induced by the dark-adaptation of the chloroplasts, suggesting an inhibition of electron exchange between Q_A and Q_B. Upon excitation of the chloroplasts with continuous light at −30°C, the A band oscillated with a periodicity of 4 with maxima at preflash numbers 2 and 6. At pH 7.5, the period-4 oscillation was converted into a period-2 oscillation by thorough dark-adaptation of the chloroplasts (24 h). Model calculations of the oscillatory patterns suggest that the period-4 oscillations of the Z_V and A bands are determined by the concentrations [S₀] + [S₁] and [S₂] + [S₃], respectively, which are present after the preflashes prior to the low-temperature continuous illumination. The period-2 oscillations in the amplitudes of the Z_V and A bands reflect the changes occurring in the redox state of the Q_B pool in a sequence of flashes. The possible relationship between the characteristics of the Z_V and A bands and the temperature-dependence of the S state transitions was investigated. Comparison of the amplitudal changes of the B (S₂Q⁻_B and S₃Q⁻_B recombination) and Q (S₂Q⁻_A recombination) thermoluminescence bands as a function of the excitation temperature suggests that the S₂ → S₃ and S₃ → S₄ transitions are blocked at about −65 and −40°C, respectively. It is also concluded that the thermoluminescence intensity emitted by the reaction center is about twice as high in the S₃ state as in the S₂ state.     

Damping of oscillations in the semiquinone absorption in reaction centers after successive flashes. Determination of the equilibrium between QA−QB and QAQB−

A quantitative model for the damping of oscillations of the semiquinone absorption after successive light flashes is presented. It is based on the equilibrium between the states Q_A^?Q_B and Q_AQ_B^?. A fit of the model to the experimental results obtained for reaction centers from Rhodopseudomonas sphaeroides gave a value of $\text{α =}\text{[}\text{Q}{}_{\mathrm{<mtext>A</mtext>}}{}^{\mathrm{?}}\text{Q}{}_{\mathrm{<mtext>B</mtext>}}\text{]}\text{([}\text{Q}{}_{\mathrm{<mtext>A</mtext>}}{}^{\mathrm{?}}\text{Q}{}_{\mathrm{<mtext>B</mtext>}}\text{] + [}\text{Q}{}_{\mathrm{<mtext>A</mtext>}}\text{Q}{}_{\mathrm{<mtext>B</mtext>}}{}^{\mathrm{?}}\text{])}\text{= 0.065 ± 0.005}$ (T = 21°C, pH 8).     

Effects of photoinhibition on the PS II acceptor side including the endogenous high spin Fe2+ in thylakoids,PS II-membrane fragments and PS II core complexes

Effects of photoinhibition at 0 °C on the PS II acceptor side have been analyzed by comparative studies in isolated thylakoids, PS II membrane fragments and PS II core complexes from spinach under conditions where degradation of polypeptide(s) D1(D2) is highly retarded. The following results were obtained by measurements of the transient fluorescence quantum and oxygen yield, respectively, induced by a train of short flashes in dark-adapted samples: (a) in the control the decay of the fluorescence quantum yield is very rapid after the first flash, if the dark incubation was performed in the presence of 300 M K₃[Fe(CN)₆]; whereas, a characteristic binary oscillation was observed in the presence of 100 M phenyl-p-benzoquinone with a very fast relaxation after the even flashes (2nd, 4th. . . ) of the sequence; (b) illumination of the samples in the presence of K₃[Fe(CN)₆] for only 5 min with white light (180 W m^-2) largely eliminates the very fast fluorescence decay after the first flash due to Q_A ^- reoxidation by preoxidized endogenous non-heme Fe³⁺, while a smaller effect arises on the relaxation kinetics of the fluorescence transients induced by the subsequent flashes; (c) the extent of the normalized variable fluorescence due to the second (and subsequent) flash(es) declines in all sample types with a biphasic time dependence at longer illumination. The decay times of the fast (6–9 min) and the slow degradation component (60–75 min) are practically independent of the absence or presence of K₃[Fe(CN)₆] and of anaerobic and aerobic conditions during the photo-inhibitory treatment, while the relative extent of the fast decay component is higher under anaerobic conditions. (d) The relaxation kinetics of the variable fluorescence induced by the second (and subsequent) flash(es) become retarded due to photoinhibition, and (e) the oscillation pattern of the oxygen yield caused by a flash train is not drastically changed due to photoinhibition.Based on these findings, it is concluded that photoinhibition modifies the reaction pattern of the PS II acceptor side prior to protein degradation. The endogenous high spin Fe²⁺ located between Q_A and Q_B is shown to become highly susceptible to modification by photoinhibition in the presence of K₃[Fe(CN)₆] (and other exogenous acceptors), while the rate constant of Q_A ^- reoxidation by Q_B(Q_B ^-) and other acceptors (except the special reaction via Fe³⁺) is markedly less affected by a short photoinhibition. The equilibrium constant between Q_A ^- and Q_B(Q_B ^-) is not drastically changed as reflected by the damping parameters of the oscillation pattern of oxygen evolution.     

Binding and release kinetics of inhibitors of Q−A oxidation in thylakoid membranes

Oxygen flash yield patterns of dark adapted thylakoid membranes as measured with a Joliot-type O₂-electrode indicate that inhibitors that block the oxidation of the reduced primary quinone Q^?_A of Photosystem II vary greatly in the rate of binding to and release from the inhibitor / Q_B binding environment. The ‘classical’ Photosystem-II herbicides like diuron and atrazine exhibit slow binding and release kinetics, whereas, for example, phenolic inhibitors, o-phenanthroline and synthetic quinones are exchanging quite rapidly with Q_B (about once per second or faster at inhibitor concentrations causing about 50% inhibition of O₂ evolution). No general relationship between the efficiency of the inhibitor and the exchange rate is observed; it depends mainly on the type of inhibitor. Based on the classical Kok model, equations are derived in order to calculate oxygen yields evolved by thylakoids in single-turnover flashes as a function of the rate constants of inhibitor binding to and release from the inhibitor / Q_B binding environment in the presence of an oxidized or semireduced Q_A · Q_B or Q_A · inhibitor complex. Fitting of theoretical and experimental values yields that o-phenanthroline binds much faster to an oxidized than to a semireduced Q_A · Q_B complex. This fits very well with the hypothesis that the Q^?_B affinity to the site is much higher than that of Q_B. In the case of i-dinoseb, however, inhibitor / quinone exchange seems to occur mainly in the semiquinone state. Possibilities to explain this result are discussed.     

Kinetics and thermodynamics of the P870+Q−A → P870+Q−B reaction in isolated reaction centers from the photosynthetic bacterium Rhodopseudomonas sphaeroides

The temperature dependences of the P870⁺Q^?_A → P870Q_A and P870⁺Q^?_B → P870Q_B recombination reactions were measured in reaction centers from Rhodopseudomonas sphaeroides. The data indicate that the P870⁺Q^?_B state decays by thermal repopulation of the P870⁺Q^?_A state, followed by recombination. ΔG° for the P870⁺Q^?_A → P870⁺Q^?_B reaction is ?6.89 kJ · mol^?1, while ΔH° = ?14.45 kJ · mol^?1 and ?TΔS° = + 7.53 kJ · mol^?1. The activation ethalpy, $\text{H}{}^3$, for the P870⁺Q^?_A Δ P870⁺Q^?_B reaction is +56.9 kJ · mol^?1, while the activation entropy is near zero. The results permit an estimate of the shape of the potential energy curve for the P870⁺Q^?_A → P870⁺Q^?_B electron transfer reaction.     

Peroxynitrite inhibits electron transport on the acceptor side of higher plant photosystem II

Peroxynitrite is a strong oxidant that has been proposed to form in chloroplasts. The interaction between peroxynitrite and photosystem II (PSII) has been investigated to determine whether this oxidant could be a hazard for PSII. Peroxynitrite is shown to inhibit oxygen evolution in PSII membranes in a dose-dependent manner. Analyses by PAM fluorimetry and EPR spectroscopy have demonstrated that the inhibition target of peroxynitrite is on the PSII acceptor side. In the presence of the herbicide DCMU, the chlorophyll (Chl) a fluorescence induction curve is inhibited by peroxynitrite, but the slow phase of the Chl a fluorescence decay does not change. EPR studies demonstrate that the Signal II_slow and Signal II_fast of peroxynitrite-treated Tris-washed PSII membranes are induced at room temperature, implying that the redox active tyrosines Y_Z and Y_D of PSII are not significantly nitrated. A featureless EPR signal with a g value of approximately 2.0043 ± 0.0003 and a line width of 10 ± 1 G is induced under continuous illumination in the presence of peroxynitrite. This new EPR signal corresponds with the semireduced plastoquinone Q_A in the absence of magnetic interaction with the non-heme Fe²⁺. We conclude that peroxynitrite impairs PSII electron transport in the Q_AFe²⁺ niche.     

Effect of different methods of Ca<Superscript>2+</Superscript> extraction from PSII oxygen-evolving complex on the Q<Subscript>A</Subscript><Superscript>−</Superscript> oxidation kinetics

Lumenal extrinsic proteins PsbO, PsbP, and PsbQ of photosystem II (PSII) protect the catalytic cluster Mn₄CaO₅ of oxygen-evolving complex (OEC) from the bulk solution and from soluble compounds in the surrounding medium. Extraction of PsbP and PsbQ proteins by NaCl-washing together with chelator EGTA is followed also by the depletion of Ca²⁺ cation from OEC. In this study, the effects of PsbP and PsbQ proteins, as well as Ca²⁺ extraction from OEC on the kinetics of the reduced primary electron acceptor (Q_A ^?) oxidation, have been studied by fluorescence decay kinetics measurements in PSII membrane fragments. We found that in addition to the impairment of OEC, removal of PsbP and PsbQ significantly slows the rate of electron transfer from Q_A ^? to the secondary quinone acceptor Q_B. Electron transfer from Q_A ^? to Q_B in photosystem II membranes with an occupied Q_B site was slowed down by a factor of 8. However, addition of EGTA or CaCl₂ to NaCl-washed PSII did not change the kinetics of fluorescence decay. Moreover, the kinetics of Q_A ^? oxidation by Q_B in Ca-depleted PSII membranes obtained by treatment with citrate buffer at pH 3.0 (such treatment keeps all extrinsic proteins in PSII but extracts Ca²⁺ from OEC) was not changed. The results obtained indicate that the effect of NaCl-washing on the Q_A ^? to Q_B electron transport is due to PsbP and PsbQ extrinsic proteins extraction, but not due to Ca²⁺ depletion.     

Evidence from thermoluminescence for bicarbonate action on the recombination reactions involving the secondary quinone electron acceptor of Photosystem II

In this paper, we present the first measurements on thermoluminescence from isolated thylakoids to probe the recombination reactions of S₂ (or possibly S₃) with Q^?_B or Q^?_A, after bicarbonate depletion and its readdition. The effects of bicarbonate depletion on the S₂Q^?_B (or S₃O^?_B) thermoluminescence band was (1) a 6–10°C shift to a higher temperature; (2) a reduction in its intensity upon prolonged depletion; and (3) elimination after the first few flashes of the characteristic period four oscillations in its intensity as a function of the flash number. On the other hand, addition of diuron (3-(3′,4′-dichlorophenyl)-1,1-dimethylurea), which blocks electron flow from Q^?_A to Q_B, produced the same thermoluminescence band, at about + 20°C, assigned to S₂Q^?_A recombination, in both depleted and reconstituted samples. These results suggest (1) the initial effect of bicarbonate depletion is to increase the activation energy for S₂(S₃)Q^?_B recombination; (2) with further depletion, the incidence of this recombination decreases and the cycling of the S₂Q^?_B and S₃Q^?_B recombination is inhibited through effects at the Q_B apoprotein; and (3) the depletion effects are fully reversible. It is suggested that a conformational change of the PS II complex in the region of the Q_B apoprotein is responsible for these effects.