Electron Transfer in the Photosynthetic Membrane: Influence of PH and Surface Potential on the P-680 Reduction Kinetics

The surface charge density of plant cell membranes (sigma): an attempt to resolve conflicting values for intrinsic sigma

The electrical potentials at membrane surfaces (psi0) strongly influence the physiological responses to ions. Ion activities at membrane surfaces may be computed from psi0, and physiological responses to ions are better interpreted with surface activities than with bulk-phase activities. psi0 influences the gating of ion channels and the driving force for ion fluxes across membranes. psi0 may be computed with electrostatic models incorporating the intrinsic surface charge density of the membrane (sigma0), the ion composition of the bathing medium, and ion binding to the membrane. Some of the parameter values needed for the models are well established: the equilibrium constants for ion binding were confirmed for several ions using multiple approaches, and a method is proposed for the computation of other binding constants. sigma0 is less well established, although it has been estimated by several methods, including computation from the near-surface electrical potentials [zeta (zeta) potentials] measured by electrophoreses. Computation from zeta potentials yields values in the range -2 mC m(-2) to -8 mC m(-2), but other methods yield values in the range -15 mC m(-2) to -40 mC m(-2). A systematic discrepancy between measured and computed zeta potentials was noted. The preponderance of evidence supports the suitability of sigma0=-30 mC m(-2). A proposed, fully paramatized Gouy-Chapman-Stern model appears to be suitable for the interpretation of many plant responses to the ionic environment.

The differences in microenvironments and functions of tyrosine radicals YZ and YD in photosystem II studied by EPR

Electron paramagnetic resonance (EPR) and electron nuclear double resonance (ENDOR) were performed to investigate the difference in microenvironments and functions between tyrosine Z (Y(Z)) and tyrosine D (Y(D)). Mn-depletion or Ca(2+)-depletion causes extension of the lifetime of tyrosine radical Y(Z)(*), which can be trapped by rapid freezing after illumination at about 250 K. Above pH 6.5, Y(Z)(*) radical in Mn-depleted PS II shows similar EPR and ENDOR spectra similar to that of Y(D)(*) radical, which are ascribed to a typical neutral tyrosine radical. Below pH 6.5, Y(Z)(*) radical shows quite different EPR and ENDOR spectra. ENDOR spectra show the spin density distribution of the low-pH form of Y(Z)(*) that has been quite different from the high-pH form of Y(Z)(*). The spin density distribution of the low-pH Y(Z)(*) can be explained by a cation radical or the neutral radical induced by strong electrostatic interaction. The pH dependence of the activation energy of the recombination rate between Y(Z)(*) and Q(A)(-) shows a gap of 4.4 kJ/mol at pH 6.0-6.5. In the Ca(2+)-depleted PS II, Y(Z)(*) signal was the mixture of the cation-like and normal neutral radicals, and the pH dependence of Y(Z)(*) spectrum in Ca(2+)-depleted PS II is considerably different from the neutral radical found in Mn-depleted PS II. Based on the recent structure data of cyanobacterial PS II, the pH dependence of Y(Z)(*) could be ascribed to the modification of the local structure and hydrogen-bonding network induced by the dissociation of ASP170 near Y(Z).

Functional Characterization of Monomeric Photosystem II Core Preparations fromThermosynechococcus elongatuswith or without the Psb27 Protein

Two monomeric fractions of photosystem II (PS II) core pacticles from the thermophilic cyanobacterium Thermosynechococcus elongatus have been investigated using flash-induced variable fluorescence kinetics and EPR spectroscopy. One fraction was highly active in oxygen evolution and contained the extrinsic protein subunits PsbO, PsbU, and PsbV. The other monomeric fraction lacked oxygen evolving activity as well as the three extrinsic subunits, but the luminally located, extrinsic Psb27 lipoprotein was present. In the monomeric fraction with bound Psb27, flash-induced variable fluorescence showed an absence of oxidizable Mn on the donor side of PS II and impaired forward electron transfer from the primary quinone acceptor, QA. These results were confirmed with EPR spectroscopy by the absence of the "split S1" interaction signal from YZ* and the CaMn4 cluster and by the absence of the S2-state multiline signal. A different protein composition on the donor side of PS II monomers with Psb27 was also supported by the lack of an EPR signal from cytochrome c550 (in the PsbV subunit). In addition, we did not observe any oxidation of cytochrome b559 at low temperature in this fraction. The presence of Psb27 and the absence of the CaMn4 cluster did not affect the protein matrix around YD or the acceptor side quinones as can be judged from the appearance of the corresponding EPR signals. The diminished electron transport capabilities on both the donor and the acceptor side of PS II when Psb27 is present give further indications that this PS II complex is involved in the earlier steps of the PS II repair cycle.

The mechanism of UV-A radiation-induced inhibition of photosystem II electron transport studied by EPR and chlorophyll fluorescence

The UV-A (320-400 nm) component of sunlight is a significant damaging factor of plant photosynthesis, which targets the photosystem II complex. Here we performed a detailed characterization of UV-A-induced damage in photosystem II membrane particles using EPR spectroscopy and chlorophyll fluorescence measurements. UV-A irradiation results in the rapid inhibition of oxygen evolution accompanied by the loss of the multiline EPR signal from the S(2) state of the water-oxidizing complex. Gradual decrease of EPR signals arising from the Q(A)(-)Fe(2+) acceptor complex, Tyr-D degrees, and the ferricyanide-induced oxidation of the non-heme Fe(2+) to Fe(3+) is also observed, but at a significantly slower rate than the inhibition of oxygen evolution and of the multiline signal. The amplitude of Signal II(fast), arising from Tyr-Z degrees in the absence of fast electron donation from the Mn cluster, was gradually increased during the course of UV-A treatment. However, the amount of functional Tyr-Z decreased to a similar extent as Tyr-D as shown by the loss of amplitude of Signal II(fast) that could be measured in the UV-A-treated particles after Tris washing. UV-A irradiation also affects the relaxation of flash-induced variable chlorophyll fluorescence. The amplitudes of the fast (600 micros) and slow (2 s) decaying components, assigned to reoxidation of Q(A)(-) by Q(B) and by recombination of (Q(A)Q(B))(-) with donor side components, respectively, decrease in favor of the 15-20 ms component, which reflects PQ binding to the Q(B) site. In the presence of DCMU, the fluorescence relaxation is dominated by a 1 s component due to recombination of Q(A)(-) with the S(2) state. After UV-A radiation, this is partially replaced by a much faster component (30-70 ms) arising from recombination of Q(A)(-) with a stabilized intermediate PSII donor, most likely Tyr-Z degrees. It is concluded that the primary damage site of UV-A irradiation is the catalytic manganese cluster of the water-oxidizing complex, where electron transfer to Tyr-Z degrees and P(680)(+) becomes inhibited. Modification and/or inactivation of the redox-active tyrosines and the Q(A)Fe(2+) acceptor complex are subsequent events. This damaging mechanism is very similar to that induced by the shorter wavelength UV-B (280-320) radiation, but different from that induced by the longer wavelength photosynthetically active light (400-700 nm).

The S(3) state of the oxygen-evolving complex in photosystem II is converted to the S(2)Y(Z)* state at alkaline pH

Here we report an EPR signal that is induced by a pH jump to alkaline pH in the S(3) state of the oxygen-evolving complex in photosystem II. The S(3) state is first formed with two flashes at pH 6. Thereafter, the pH is changed in the dark prior to freezing of the sample. The EPR signal is 90-100 G wide and centered around g = 2. The signal is reversibly induced with a pK = 8.5 +/- 0.3 and is very stable with a decay half-time of 5-6 min. If the pH is changed in the dark from pH 8.6 to 6.0, the signal disappears although the S(3) state remains. We propose that the signal arises from the interaction between the Mn cluster and Y(Z), resulting in the spin-coupled S(2)Y(Z)(*) signal. Our data suggest that the potential of the Y(Z)(*)/Y(Z) redox couple is sensitive to the ambient pH in the S(3) state. The alkaline pH decreases the potential of the Y(Z)(*)/Y(Z) couple so that Y(Z) can give back an electron to the S(3) state, thereby obtaining the S(2)Y(Z)(*) EPR signal. The tyrosine oxidation also involves proton release from Y(Z), and the results support a mechanism where this proton is released to the bulk medium presumably via a close-lying base. Thus, the equilibrium is changed from S(3)Y(Z) to S(2)Y(Z)(*) by the alkaline pH. At normal pH (pH 5.5-7), this equilibrium is set strongly to the S(3)Y(Z) state. The results are discussed in relation to the present models of water oxidation. Consequences for the relative redox potentials of Y(Z)(*)/Y(Z) and S(3)/S(2) at different pH values are discussed. We also compare the pH-induced S(2)Y(Z)(*) signal with the S(2)Y(Z)(*) signal from Ca(2+)-depleted photosystem II.

Comparative studies of the S0 and S2 multiline electron paramagnetic resonance signals from the manganese cluster in Photosystem II

Electron paramagnetic resonance (EPR) spectroscopy is one of the major techniques used to analyse the structure and function of the water oxidising complex (WOC) in Photosystem II. The discovery of an EPR signal from the S0 state has opened the way for new experiments, aiming to characterise the S0 state and elucidate the differences between the different S states. We present a review of the biochemical and biophysical characterisation of the S0 state multiline signal that has evolved since its discovery, and compare these results to previous and recent data from the S2 multiline signal. We also present some new data from the S2 state reached on the second turnover of the enzyme.

Amino acid residues that modulate the properties of tyrosine Y(Z) and the manganese cluster in the water oxidizing complex of photosystem II

The catalytic site for photosynthetic water oxidation is embedded in a protein matrix consisting of nearly 30 different polypeptides. Residues from several of these polypeptides modulate the properties of the tetrameric Mn cluster and the redox-active tyrosine residue, Y(Z), that are located at the catalytic site. However, most or all of the residues that interact directly with Y(Z) and the Mn cluster appear to be contributed by the D1 polypeptide. This review summarizes our knowledge of the environments of Y(Z) and the Mn cluster as obtained from the introduction of site-directed, deletion, and other mutations into the photosystem II polypeptides of the cyanobacterium Synechocystis sp. PCC 6803 and the green alga Chlamydomonas reinhardtii.

Electron transport through photosystem II in leaves during light pulses: acceptor resistance increases with nonphotochemical excitation quenching

Light response curves of photosystem (PS) II electron transport from oxygen evolving complex to plastoquinone (PQ) were measured in sunflower (Helianthus annuus L.), cotton (Gossypium hirsutum L.) and tobacco (Nicotiana tabacum L.) leaves by recording O(2) evolution and fluorescence in 5-200 ms light pulses of 500-13500 micromol absorbed quanta m(-2) s(-1). The leaves were pre-adapted at 60-2000 micromol quanta m(-2) s(-1) for 60 min to obtain different nonphotochemical excitation quenching, which was predominantly of reversible q(I) type (relaxation time 30 min). PQ was completely oxidized by turning the actinic light off and illuminating with far-red light for 2 s before the pulse was applied in the dark, 4 s after the actinic light was turned off. Electron transport rate calculated from fluorescence transients considering PS II donor side resistance (V. Oja, A. Laisk, submitted) was maximal at the beginning of pulses (J(Fi)) and decreased immediately. The dependences of J(Fi) on pulse absorbed flux density were rectangular hyperbolas with K(m) about 7500 micromol m(-2) s(-1). Both the extrapolated plateau J(Fm) and initial slope (intrinsic quantum yield of PS II, Y(m)) decreased proportionally when q(I) increased from minimum to maximum (J(Fm) from 2860 to 1450 micromol e(-) m(-2) s(-1) and Y(m) from 0.41 to 0.23). The time constant for electron transfer away from the PS II acceptor side, calculated from a model of PS II electron transport for 2 micromol PS II m(-2), increased from 607 to 1315 microseconds with the activation of q(I) while the donor side time constant changed from 289 to 329 microseconds. These results show that changes in the electron transfer processes on the acceptor side of PS II occur in parallel with nonphotochemical (predominantly reversible q(I) type) excitation quenching.

Proton equilibria in the manganese cluster of photosystem II control the intensities of the S(0) and S(2) state g approximately 2 electron paramagnetic resonance signals

We have studied the pH effect on the S(0) and S(2) multiline electron paramagnetic resonance (EPR) signals from the water-oxidizing complex of photosystem II. Around pH 6, the maximum signal intensities were detected. On both the acidic and alkaline sides of pH 6, the intensities of the EPR signals decreased. Two pKs were determined for the S(0) multiline signal; pK(1) = 4.2 +/- 0.2 and pK(2) = 8.0 +/- 0.1, and for the S(2) multiline signal the pKs were pK(1) = 4.5 +/- 0.1 and pK(2) = 7.6 +/- 0.1. The intensity of the S(0)-state EPR signal was partly restored when the pH was changed from acidic or alkaline pH back to pH approximately 6. In the S(2) state we observed partial recovery of the multiline signal when going from alkaline pH back to pH approximately 6, whereas no significant recovery of the S(2) multiline signal was observed when the pH was changed from acidic pH back to pH approximately 6. Several possible explanations for the intensity changes as a function of pH are discussed. Some are ruled out, such as disintegration of the Mn cluster or decay of the S states and formal Cl(-) and Ca(2+) depletion. The altered EPR signal intensities probably reflect the protonation/deprotonation of ligands to the Mn cluster or the oxo bridges between the Mn ions. Also, the possibility of decreased multiline signal intensities at alkaline pH as an effect of changed redox potential of Y(Z) is put forward.

Role of D1-His190 in the proton-coupled oxidation of tyrosine YZ in manganese-depleted photosystem II

To further characterize the role of D1-His190 in the oxidation of tyrosine Y(Z) in photosystem II, the pH dependence of P(680)(*)()(+) reduction was measured in H190A and Mn-depleted wild-type PSII particles isolated from the cyanobacterium, Synechocystis sp. PCC 6803. Measurements were conducted in the presence and absence of imidazole and other small organic bases. In H190A PSII particles, rapid reduction of P(680)(*)()(+) attributed to electron transfer from Y(Z) increased dramatically above pH 9, with an apparent pK(A) of approximately 10.3. In the presence of ethanolamine and imidazole, this dramatic increase occurred at lower pH values, with the efficiency of Y(Z) oxidation correlating with the solution pK(A) value of the added base. We conclude that the pK(A) of Y(Z) is approximately 10.3 in D1-H190A PSII particles. In Mn-depleted wild-type PSII particles, P(680)(*)()(+) reduction was accelerated by all exogenous bases examined (substituted imidazoles, histidine, Tris, and 1,4-diazabicyclo[2.2.2]octane). We conclude that Y(Z) is solvent accessible in Mn-depleted wild-type PSII particles and that its pK(A) is near that of tyrosine in solution. In Mn-depleted wild-type PSII particles, over 80% of the kinetics of P(680)(*)()(+) reduction after a flash could be described by three kinetic components. The individual rate constants of these components varied slightly with pH, but their relative proportions varied dramatically with pH, showing apparent pK(A) values of 7.5 and 6.25 (6.9 and 5.8 in the presence of Ca(2+) and Mg(2+) ions). An additional pK(A) value (pK(A) < 4.5) may also be present. To describe these data, we propose (1) the pK(A) of His190 is 6.9-7.5, depending on buffer ions, (2) the deprotonation of Y(Z) is facilitated by the transient formation of a either a hydrogen bond or a hydrogen-bonded water bridge between Y(Z) and D1-His190, and (3) when protonated, D1-His190 interacts with nearby residues having pK(A) values near 6 and 4. Because Y(Z) and D1-His190 are located near the Mn cluster, these residues may interact with the Mn cluster in the intact system.

A new electrochemical gradient generator in thylakoid membranes of green algae

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

Involvement of histidine 190 on the D1 protein in electron/proton transfer reactions on the donor side of photosystem II

Flash-induced chlorophyll fluorescence kinetics from photosystem II in thylakoids from the dark-grown wild type and two site-directed mutants of the D1 protein His190 residue (D1-H190) in Chlamydomonas reinhardtii have been characterized. Induction of the chlorophyll fluorescence on the first flash, reflecting electron transport from YZ to P680(+), exhibited a strong pH dependence with a pK of 7.6 in the dark-grown wild type which lacks the Mn cluster. The chlorophyll fluorescence decay, measured in the presence of DCMU, which reflects recombination between QA- and YZox, was also pH-dependent with a similar pK of 7.5. These results indicate participation by the same base, which is suggested to be D1-H190, in oxidation and reduction of YZ in forward electron transfer and recombination pathways, respectively. This hypothesis was tested in the D1-H190 mutants. Induction of chlorophyll fluorescence in these H190 mutants has been observed to be inefficient due to slow electron transfer from YZ to P680(+) [Roffey, R. A., et al. (1994) Biochim. Biophys. Acta 1185, 257-270]. We show that this reaction is pH-dependent, with a pK of 8. 1, and at pH >/=9, the fluorescence induction is efficient in the H190 mutants, suggesting direct titration of YZ. The efficient oxidation of YZ ( approximately 70% at pH 9.0) at high pH was confirmed by kinetic EPR measurements. In contrast to the wild type, the H190 mutants show little or no observable fluorescence decay. Our data suggest that H190 is an essential component in the electron transfer reactions in photosystem II and acts as a proton acceptor upon YZ oxidation. In the H190 mutants, this reaction is inefficient and YZ oxidation only occurs at elevated pHs when YZ itself probably is deprotonated. We also propose that H190 is able to return a proton to YZox during electron recombination from QA- in a reaction which does not take place in the D1-H190 mutants.

Role of D1-His190 in proton-coupled electron transfer reactions in photosystem II: a chemical complementation study

Recent models for water oxidation in photosystem II propose that His190 of the D1 polypeptide facilitates electron transfer from tyrosine YZ to P680+ by accepting the hydroxyl proton from YZ. To test these models, and to further define the role of D1-His190 in the proton-coupled electron transfer reactions of PSII, the rates of P680+ reduction, YZ oxidation, QA- oxidation, and YZ* reduction were measured in PSII particles isolated from several D1-His190 mutants constructed in the cyanobacterium Synechocystis sp. PCC 6803. These measurements were conducted in the absence and presence of imidazole and other small organic bases. In all mutants examined, the rates of P680+ reduction, YZ oxidation, and YZ* reduction after a single flash were slowed dramatically and the rate of QA- oxidation was accelerated to values consistent with the reduction of P680+ by QA- rather than by YZ. There appeared to be little correlation between these rates and the nature of the residue substituted for D1-His190. However, in nearly all mutants examined, the rates of P680+ reduction, YZ oxidation, and YZ* reduction were accelerated dramatically in the presence of imidazole and other small organic bases (e.g., methyl-substituted imidazoles, histidine, methylamine, ethanolamine, and TRIS). In addition, the rate of QA- oxidation was decelerated substantially. For example, in the presence of 100 mM imidazole, the rate of electron transfer from YZ to P680+ in most D1-His190 mutants increased 26-87-fold. Furthermore, in the presence of 5 mM imidazole, the rate of YZ* reduction in the D1-His190 mutants increased to values comparable to that of Mn-depleted wild-type PSII particles in the absence of imidazole. On the basis of these results, we conclude that D1-His190 is the immediate proton acceptor for YZ and that the hydroxyl proton of YZ remains bound to D1-His190 during the lifetime of YZ*, thereby facilitating the reduction of YZ*.

Stabilization of charge separation and photochemical misses in photosystem II

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

Function of tyrosine Z in water oxidation by photosystem II: electrostatical promotor instead of hydrogen abstractor

Photosynthetic water oxidation by photosystem II is mediated by a Mn4 cluster, a cofactor X still chemically ill-defined, and a tyrosine, YZ (D1-Tyr161). Before the final reaction with water proceeds to yield O2 (transition S4-->S0), two oxidizing equivalents are stored on Mn4 (S0-->S1-->S2), a third on X (S2-->S3), and a forth on YZ(S3-->S4). It has been proposed that YZ functions as a pure electron transmitter between Mn4X and P680, or, more recently, that it acts as an abstractor of hydrogen from bound water. We scrutinized the coupling of electron and proton transfer during the oxidation of YZ in PSII core particles with intact or impaired oxygen-evolving capacity. The rates of electron transfer to P680+, of electrochromism, and of pH transients were determined as a function of the pH, the temperature, and the H/D ratio. In oxygen-evolving material, we found only evidence for electrostatically induced proton release from peripheral amino acid residues but not from YZox itself. The positive charge stayed near YZox, and the rate of electron transfer was nearly independent of the pH. In core particles with an impaired Mn4 cluster, on the other hand, the rate of the electron transfer became strictly dependent on the protonation state of a single base (pK approximately 7). At pH < 7, the rate of electron transfer revealed the same slow rate (t1/2 approximately 35 microseconds) as that of proton release into the bulk. The deposition of a positive charge around YZox was no longer detected. A large H/D isotope effect (approximately 2.5) on these rates was also indicative of a steering of electron abstraction by proton transfer. That YZox was deprotonated into the bulk in inactive but not in oxygen-evolving material argues against the proposed role of YZox as an acceptor of hydrogen from water. Instead, the positive charge in its vicinity may shift the equilibrium from bound water to bound peroxide upon S3-->S4 as a prerequisite for the formation of oxygen upon S4-->S0.

Charge recombination and proton transfer in manganese-depleted photosystem II

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

Photochemical reactions of photosystem II in ethylene glycol

The behavior of photosystem II (PSII) reactions was investigated under conditions of decreasing water content by the addition of increasing concentrations of ethylene glycol (EG). The photosynthetic activities were measured for PSII samples either directly in aqueous solutions of EG or in the standard buffer medium following EG treatment. Several effects on PSII arise upon exposure to EG. Below 50% EG there are no significant irreversible changes, although there is a slowing of the QA-reoxidation kinetics in the presence of EG. At concentrations of 50-70% EG, protein structural changes occur that include the release of the 16, 23, and 33 kDa extrinsic proteins and two of the catalytic Mn ions. For these samples, the capacity for O2 evolution is considerably reduced and the formation of donor side H2O2 is enhanced. In 60% EG, the nanosecond components in the rate of P680+ reduction are converted entirely to microsecond kinetics which upon return of the sample to the standard buffer medium are partially restored, indicating that EG has a reversible, solvent effect on the PSII donor side. At concentrations of EG > 70% chlorophyll fluorescence measurements reveal reversible increases in the FO level concomitant with the generation and disappearance of a 5 microseconds decay component in the P680+ reduction kinetics. This result may indicate a solvent-induced uncoupling of the light harvesting pigment bed from the reaction center complex. As the EG concentration is increased to 80-100%, there is an irreversible loss of the primary charge separation. The use of EG as a cryoprotectant and as a water-miscible organic solvent for PSII is discussed.

A model for the photosystem II reaction center core including the structure of the primary donor P680

For a detailed understanding of the function of photosystem II (PSII), a molecular structure is needed. The crystal structure has not yet been determined, but the PSII reaction center proteins D1 and D2 show homology with the L and M subunits of the photosynthetic reaction center from purple bacteria. We have modeled important parts of the D1 and D2 proteins on the basis of the crystallographic structure of the reaction center from Rhodopseudomonas viridis. The model contains the central core of the PSII reaction center, including the protein regions for the transmembrane helices B, C, D, and E and loops B-C and C-D connecting the helices. In the model, four chlorophylls, two pheophytins, and the nonheme Fe2+ ion are included. We have applied techniques from computational chemistry that incorporate statistical data on side-chain rotameric states from known protein structure and that describe interactions within the model using an empirical potential energy function. The conformation of chlorophyll pigments in the model was optimized by using exciton interaction calculations in combination with potential energy calculations to find a solution that agrees with experimentally determined exciton interaction energies. The model is analyzed and compared with experimental results for the regions of P680, the redox active pheophytin, the acceptor side Fe2+, and the tyrosyl radicals TyrD and TyrZ. P680 is proposed to be a weakly coupled chlorophyll a pair which makes three hydrogen bonds with residues on the D1 and D2 proteins. In the model the redox-active pheophytin is hydrogen bonded to D1-Glu130 and possibly also to D1-Tyr126 and D1-Tyr147. TyrD is hydrogen bonded to D2-His190 and also interacts with D2-Gln165. TyrZ is bound in a hydrophilic environment which is partially constituted by D1-Gln165, D1-Asp170, D1-Glu189, and D1-His190. These polar residues are most likely involved in proton transfer from oxidized TyrZ or in metal binding.

P680(+) reduction in oxygen-evolving Photosystem II core complexes

The kinetics of P680(+) reduction in oxygen-evolving spinach Photosystem II (PS II) core particles were studied using both repetitive and single-flash 830 nm transient absorption. From measurements on samples in which PS II turnover is blocked, we estimate radical-pair lifetimes of 2 ns and 19 ns. Nanosecond single-flash measurements indicate decay times of 7 ns, 40 ns and 95 ns. Both the longer 40 ns and 95 ns components relate to the normal S-state controlled Yz → P680(+) electron transfer dynamics. Our analysis indicates the existence of a 7 ns component which provides evidence for an additional process associated with modified interactions involving the water-splitting catalytic site. Corresponding microsecond measurements show decay times of 4 μs and 90 μs with the possibility of a small component with a decay time of 20-40 μs. The precise origin of the 4 μs component remains uncertain but appears to be associated with the water-splitting center or its binding site while the 90 μs component is assigned to P680(+)-QA (-) recombination. An amplitude and kinetic analysis of the flash dependence data gives results that are consistent with the current model of the oxygen-evolving complex.

Photoinhibition of photosystem II in vivo is preceded by down-regulation through light-induced acidification of the lumen: Consequences for the mechanism of photoinhibition in vivo

The mechanism of photoinhibition of photosystem II (PSII) was studied in intact leaf discs of Spinacia oleracea L. and detached leaves of Vigna unguiculata L. The leaf material was exposed to different photon flux densities (PFDs) for 100 min, while non-photochemical (qN) and photochemical quenching (qp) of chlorophyll fluorescence were monitored. The 'energy' and redox state of PSII were manipulated quite independently of the PFD by application of different temperatures (5-20° C), [CO2] and [O2] at different PFDs. A linear or curvilinear relationship between qp and photoinhibition of PSII was observed. When [CO2] and [O2] were both low (30 μl · l(-1) and 2%, respectively), PSII was less susceptible at a given qp than at ambient or higher [CO2] and photoinhibition became only substantial when qp decreased below 0.3. When high levels of energy-dependent quenching (qE) (between 0.6 and 0.8) were reached, a further increase of the PFD or a further decrease of the metabolic demand for ATP and NADPH led to a shift from qE to photoinhibitory quenching (qI). This shift indicated that photoinhibition was preceded by down-regulation through light-induced acidification of the lumen. We propose that photoinhibition took place in the centers down-regulated by qE. The shift from qE to qI occurred concomitant with qP decreasing to zero. The results clearly show that photoinhibition does not primarily depend on the photon density in the antenna, but that photoinhibition depends on the energy state of the membrane in combination with the redox balance of PSII. The results are discussed with regard to the mechanism of photoinhibition of PSII, considering, in particular, effects of light-induced acidification on the donor side of PSII. Interestingly, cold-acclimation of spinach leaves did not significantly affect the relationship between qP, qE and photoinhibition of PSII at low temperature.

Kinetic factors in the bicycle model of oxygen evolution by Photosystem II

Flash-induced oxygen evolution and many related processes in thylakoids of oxygenic organisms are modulated with period four by the S-state transitions associated with the oxygen evolving system of Photosystem II (PS II). To analyze these phenomena, we have interpreted the S-state model on the basis of the charge accumulating activities on both sides of PS II-4 charges on the donor side and 2 charges on the acceptor side. This results in the recognition of two parallel reaction center cycles V and W of PS II function (V.P. Shinkarev and C.A. Wraight (1993) Proc Natl Acad Sci USA 90: 1834-1838). The description of damping of the period four oscillations is here extended to include kinetic sources of misses in both cycles. Such misses arise in reaction centers (RCs) in which back reaction between P(+) and QA (-) occurs before the electron transfer equilibria on the donor and acceptor sides of the RC are reached. These are in addition to misses which are determined by reaction centers (RCs) that are inactive at the time of the flash due to the presence of either P(+) or QA (-) according to the electron transfer equilibria on the donor and acceptor sides of the RC. Using known or estimated values of the equilibrium and rate constants for donor and acceptor side reactions of the RC, this provides a natural and quantitatively reasonable description of the flash number dependence of oxygen evolution and other period four modulated processes of PS II. The estimated miss factors are different for both cycles V and W and are dependent on flash number and pH. Estimates based on existing data show that miss factors of the first type (kinetic) are dominant at low pH, while those of the second type (equilibrium) are dominant at high pH.

Proton release during the redox cycle of the water oxidase

Old and very recent experiments on the extent and the rate of proton release during the four reaction steps of photosynthetic water oxidation are reviewed. Proton release is discussed in terms of three main sources, namely the chemical production upon electron abstraction from water, protolytic reactions of Mn-ligands (e.g. oxo-bridges), and electrostatic response of neighboring amino acids. The extent of proton release differs between the four oxidation steps and greatly varies as a function of pH both, but differently, in thylakoids and PS II-membranes. Contrastingly, it is about constant in PS II-core particles. In any preparation, and on most if not all reaction steps, a large portion of proton transfer can occur very rapidly (<20 μs) and before the oxidation of the Mn-cluster by Yz (+) is completed. By these electrostatically driven reactions the catalytic center accumulates bases. An additional slow phase is observed during the oxygen evolving step, S3⇒S4→S0. Depending on pH, this phase consists of a release or an uptake of protons which accounts for the balance between the number of preformed bases and the four chemically produced protons. These data are compatible with the hypothesis of concerted electron/proton-transfer to overcome the kinetic and energetic constraints of water oxidation.

Inhibition of tyrosine Z photooxidation after formation of the S3 state in Ca(2+)-depleted and Cl(-)-depleted photosystem II

Ca2+ and Cl- are obligatory cofactors in photosystem II (PS-II), the oxygen-evolving enzyme of plants. The sites of inhibition in both Ca(2+)- and Cl(-)-depleted PS-II were compared using EPR and flash absorption spectroscopies to follow the extent of the photooxidation of the redox-active tyrosine (TyrZ) and of the primary electron donor chlorophyll (P680) and their subsequent reduction in the dark. The inhibition occurred after formation of the S3 state in Ca(2+)-depleted PS-II. In Cl(-)-depleted photosystem II, the inhibition occurred after formation of the S3 state in about half of the centers and probably after S2TyrZ+ formation in the remaining centers. After the S3 state was formed in Ca(2+)- and Cl(-)-depleted photosystem II, electron transfer from TyrZ to P680 was inhibited. This inhibition is discussed in terms of electrostatic constraints resulting from S3 formation in the absence of Ca2+ and Cl-.

Interactions of iodide ions with isolated photosystem 2 particles

The effects of I- ions on O2 evolution by photosystem 2 particles, which were depleted of the 18-kDa and the 23-kDa extrinsic proteins of the O2 evolution complex by NaCl washing (dPS2 particles) were examined. In the absence of Cl- (incompetent dPS2) I- stimulated O2 evolution up to 3-6 mM, depending on the associated cation, and inhibited it at higher concentrations. In the presence of Cl- (competent dPS2), I- was inhibitory at all concentrations. The inhibition was reversible, it occurred at a site preceding Tyrz (Tyr residue mediating electron transfer from H2O to photosystem 2), and it interfered noncompetitively with the reactivation of incompetent dPS2 with Cl-. Furthermore, the organic salts tetrabutyl ammonium iodide and tetraphenyl phosphonium iodide proved to be stronger inhibitors than the inorganic NaI. This is interpreted as an indication of a negatively charged surface, situated behind a hydrophobic permeability barrier. Permeant organic cations, being better compensators of the inner surface charge than Na+, are also more apt in facilitating access of the I- ions to the inhibitory site in the vicinity of Tyrz.

Current perceptions of Photosystem II

In the last few years our knowledge of the structure and function of Photosystem II in oxygen-evolving organisms has increased significantly. The biochemical isolation and characterization of essential protein components and the comparative analysis from purple photosynthetic bacteria (Deisenhofer, Epp, Miki, Huber and Michel (1984) J Mol Biol 180: 385-398) have led to a more concise picture of Photosystem II organization. Thus, it is now generally accepted that the so-called D1 and D2 intrinsic proteins bind the primary reactants and the reducing-side components. Simultaneously, the nature and reaction kinetics of the major electron transfer components have been further clarified. For example, the radicals giving rise to the different forms of EPR Signal II have recently been assigned to oxidized tyrosine residues on the D1 and D2 proteins, while the so-called Q400 component has been assigned to the ferric form of the acceptor-side iron. The primary charge-separation has been meaured to take place in about 3 ps. However, despite all recent major efforts, the location of the manganese ions and the water-oxidation mechanism still remain largely unknown. Other topics which lately have received much attention include the organization of Photosystem II in the thylakoid membrane and the role of lipids and ionic cofactors like bicarbonate, calcium and chloride. This article attempts to give an overall update in this rapidly expanding field.

Mn(2+) 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 Mn(2+). Using flash photolysis with electron spin resonance detection, we examined the room-temperature reaction kinetics of these reductants with Yz (+), 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 Yz (+) reduction by benzidine was a linear function of benzidine concentration. The rate of Yz (+) reduction by Mn(2+) at pH 6 increased linearly at low Mn(2+) concentrations and reached a maximum at the Mn(2+) concentrations equal to several times the reaction center concentration. The rate was inhibited by K(+), Ca(2+) and Mg(2+). 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 Yz (+) reduction at pH 7.5 was biphasic with a fast 400 μs phase that suggests binding of Mn(2+) near Yz (+) at a site that may be one of the native manganese binding sites.

Glycocalyx electrostatic potential profile analysis: ion, pH, steric, and charge effects

The Poisson-Boltzmann equation is modified to consider charge ionogenicity, steric exclusion, and charge distribution in order to describe the perimembranous electrostatic potential profile in a manner consistent with the known morphology and biochemical composition of the cell's glycocalyx. Exact numerical and approximate analytical solutions are given for various charge distributions and for an extended form of the Donnan potential model. The interrelated effects of ionic conditions, bulk pH, ion binding, local dielectric, steric volume exclusion, and charge distribution on the local potential, pH, and charge density within the glycocalyx are examined. Local charge-induced, potential-mediated pH reductions cause glycocalyx charge neutralization. Under certain conditions, local potentials may be insensitive to ionic strength or may decrease in spite of increasing charge density. The volume exclusion of the glycocalyx reduces the local ion concentration, thereby increasing the local potential. With neutral lipid membranes, the Donnan and surface potential agree if the glycocalyx charge distribution is both uniform and several times thicker than the Debye length (approximately 20 A in thickness under physiological conditions). Model limitations in terms of application to microdomains or protein endo- and ectodomains are discussed.

Studies on the protolytic reactions coupled with water cleavage in photosystem II membrane fragments from spinach

The protolytic reactions of PSII membrane fragments were analyzed by measurements of absorption changes of the water soluble indicator dye bromocresol purple induced by a train of 10 μs flashes in dark-adapted samples. It was found that: a) in the first flash a rapid H(+)-release takes place followed by a slower H(+)-uptake. The deprotonation is insensitive to DCMU but is completely eliminated by linolenic acid treatment of the samples; b) the extent of the H(+)-uptake in the first flash depends on the redox potential of the suspension. In this time domain no H(+)-uptake is observed in the subsequent flashes; c) the extent of the H(+)-release as a function of the flash number in the sequence exhibits a characteristic oscillation pattern. Multiphasic release kinetics are observed. The oscillation pattern can be satisfactorily described by a 1, 0, 1, 2 stoichiometry for the redox transitions Si → Si+1 (i=0, 1, 2, 3) in the water oxidizing enzyme system Y. The H(+)-uptake after the first flash is assumed to be a consequence of the very fast reduction of oxidized Q400(Fe(3+)) formed due to dark incubation with K3[Fe(CN)6]. The possible participation of component Z in the deprotonation reactions at the PSII donor side is discussed.