Role of Arg180 of the D2 protein in photosystem II structure and function

Acquirement of water-splitting ability and alteration of the charge-separation mechanism in photosynthetic reaction centers

In photosynthetic reaction centers from purple bacteria (PbRC) and the water-oxidizing enzyme, photosystem II (PSII), charge separation occurs along one of the two symmetrical electron-transfer branches. Here we report the microscopic origin of the unidirectional charge separation, fully considering electron-hole interaction, electronic coupling of the pigments, and electrostatic interaction with the polarizable entire protein environments. The electronic coupling between the pair of bacteriochlorophylls is large in PbRC, forming a delocalized excited state with the lowest excitation energy (i.e., the special pair). The charge-separated state in the active branch is stabilized by uncharged polar residues in the transmembrane region and charged residues on the cytochrome c ₂ binding surface. In contrast, the accessory chlorophyll in the D1 protein (Chl_D1) has the lowest excitation energy in PSII. The charge-separated state involves Chl_D1 ^•+ and is stabilized predominantly by charged residues near the Mn₄CaO₅ cluster and the proceeding proton-transfer pathway. It seems likely that the acquirement of water-splitting ability makes Chl_D1 the initial electron donor in PSII.

Microsolvation of the Redox-Active Tyrosine-D in Photosystem II: Correlation of Energetics with EPR Spectroscopy and Oxidation-Induced Proton Transfer

Photosystem II (PSII) of oxygenic photosynthesis captures sunlight to drive the catalytic oxidation of water and the reduction of plastoquinone. Among the several redox-active cofactors that participate in intricate electron transfer pathways there are two tyrosine residues, YZ and YD. They are situated in symmetry-related electron transfer branches but have different environments and play distinct roles. YZ is the immediate oxidant of the oxygen-evolving Mn4CaO5 cluster, whereas YD serves regulatory and protective functions. The protonation states and hydrogen-bond network in the environment of YD remain debated, while the role of microsolvation in stabilizing different redox states of YD and facilitating oxidation or mediating deprotonation, as well the fate of the phenolic proton, is unclear. Here we present detailed structural models of YD and its environment using large-scale quantum mechanical models and all-atom molecular dynamics of a complete PSII monomer. The energetics of water distribution within a hydrophobic cavity adjacent to YD are shown to correlate directly with electron paramagnetic resonance (EPR) parameters such as the tyrosyl g-tensor, allowing us to map the correspondence between specific structural models and available experimental observations. EPR spectra obtained under different conditions are explained with respect to the mode of interaction of the proximal water with the tyrosyl radical and the position of the phenolic proton within the cavity. Our results revise previous models of the energetics and build a detailed view of the role of confined water in the oxidation and deprotonation of YD. Finally, the model of microsolvation developed in the present work rationalizes in a straightforward way the biphasic oxidation kinetics of YD, offering new structural insights regarding the function of the radical in biological photosynthesis.

Energetics of the Proton Transfer Pathway for Tyrosine D in Photosystem II

The proton transfer pathway for redox active tyrosine D (TyrD) in photosystem II is a hydrogen-bond network that involves D2-Arg180 and a series of water molecules. Using quantum mechanical/molecular mechanical calculations, the detailed properties of the energetics and structural geometries were investigated. The potential-energy profile of all hydrogen bonds along the proton transfer pathway indicates that the overall proton transfer from TyrD is energetically downhill. D2-Arg180 plays a key role in the proton transfer pathway, providing a driving force for proton transfer, maintaining the hydrogen-bond network structure, stabilising P680•+, and thus deprotonating TyrD-OH to TyrD-O•. A hydrophobic environment near TyrD enhances the electrostatic interactions between TyrD and redox active groups, e.g. P680 and the catalytic Mn4CaO5 cluster: the redox states of those groups are linked with the protonation state of TyrD, i.e. release of the proton from TyrD. Thus, the proton transfer pathway from TyrD may ultimately contribute to the conversion of S0 into S1 in the dark in order to stabilise the Mn4CaO5 cluster when the photocycle is interrupted in S0.

Infrared Detection of a Proton Released from Tyrosine YD to the Bulk upon Its Photo-oxidation in Photosystem II

Photosystem II (PSII) has two symmetrically located, redox-active tyrosine residues, YZ and YD. Whereas YZ mediates the electron transfer from the water-oxidizing center to P680 in the main electron transfer pathway, YD functions as a peripheral electron donor to P680. To understand the mechanism of this functional difference between YZ and YD, it is essential to know where the proton is transferred upon its oxidation in the proton-coupled electron transfer process. In this study, we used Fourier transform infrared (FTIR) spectroscopy to examine whether the proton from YD is released from the protein into the bulk. The proton detection method previously used for water oxidation in PSII [Suzuki et al. (2009) J. Am. Chem. Soc. 131, 7849-7857] was applied to YD; a proton released into the bulk upon YD oxidation was trapped by a high-concentration Mes buffer, and the protonation reaction of Mes was monitored by FTIR difference spectroscopy. It was shown that 0.84 ± 0.10 protons are released into the bulk by oxidation of YD in one PSII center. This result indicates that the proton of YD is not transferred to the neighboring D2-His198 but is released from the protein; this is in sharp contrast to the YZ reaction, in which a proton is transferred to D1-His190 through a strong hydrogen bond. This functional difference is caused by differences in the hydrogen-bonded structures of YD and YZ, which are determined by the hydrogen bond partners at the Nπ sites of these His residues, i.e., D2-Arg294 and D1-Asn298, which function as a hydrogen bond donor and acceptor, respectively. This FTIR spectroscopy result supports the recent theoretical prediction [Saito et al. (2013) Proc. Natl. Acad. Sci. U.S.A. 110, 7690-7695] based on the X-ray crystallographic structure of PSII and explains the different rates of the redox reactions of YD and YZ.

Proton transfer reactions and hydrogen-bond networks in protein environments

In protein environments, proton transfer reactions occur along polar or charged residues and isolated water molecules. These species consist of H-bond networks that serve as proton transfer pathways; therefore, thorough understanding of H-bond energetics is essential when investigating proton transfer reactions in protein environments. When the pKa values (or proton affinity) of the H-bond donor and acceptor moieties are equal, significantly short, symmetric H-bonds can be formed between the two, and proton transfer reactions can occur in an efficient manner. However, such short, symmetric H-bonds are not necessarily stable when they are situated near the protein bulk surface, because the condition of matching pKa values is opposite to that required for the formation of strong salt bridges, which play a key role in protein-protein interactions. To satisfy the pKa matching condition and allow for proton transfer reactions, proteins often adjust the pKa via electron transfer reactions or H-bond pattern changes. In particular, when a symmetric H-bond is formed near the protein bulk surface as a result of one of these phenomena, its instability often results in breakage, leading to large changes in protein conformation.

Mechanism of tyrosine D oxidation in Photosystem II

Using quantum mechanics/molecular mechanics calculations and the 1.9-Å crystal structure of Photosystem II [Umena Y, Kawakami K, Shen J-R, Kamiya N (2011) Nature 473(7345):55-60], we investigated the H-bonding environment of the redox-active tyrosine D (TyrD) and obtained insights that help explain its slow redox kinetics and the stability of TyrD(•). The water molecule distal to TyrD, located ~4 Å away from the phenolic O of TyrD, corresponds to the presence of the tyrosyl radical state. The water molecule proximal to TyrD, in H-bonding distance to the phenolic O of TyrD, corresponds to the presence of the unoxidized tyrosine. The H(+) released on oxidation of TyrD is transferred to the proximal water, which shifts to the distal position, triggering a concerted proton transfer pathway involving D2-Arg180 and a series of waters, through which the proton reaches the aqueous phase at D2-His61. The water movement linked to the ejection of the proton from the hydrophobic environment near TyrD makes oxidation slow and quasiirreversible, explaining the great stability of the TyrD(•). A symmetry-related proton pathway associated with tyrosine Z is pointed out, and this is associated with one of the Cl(-) sites. This may represent a proton pathway functional in the water oxidation cycle.

Influence of the axial ligand on the cationic properties of the chlorophyll pair in photosystem II from Thermosynechococcus vulcanus

Influence of the axial ligand of PD1 chlorophyll (D1-His-198) on the Em of monomer chlorophylls PD1 and PD2, and the PD1•+/PD2•+ charge ratio was investigated by theoretical calculations using the PSII crystal structure of Thermosynechococcus vulcanus analyzed at 1.9-Å resolution. It was found that the Em(PD1)/Em(PD2) values and PD1•+/PD2•+ ratio remained unchanged upon D1-H198Q mutation. However, Em(PD1) was increased in the D1-H198A mutant, resulting in a more even distribution of the positive charge over PD1/PD2. Introduction of a water molecule as an axial ligand resulted in equal Em values and PD1•+/PD2•+ ratios between the mutant and wild-type, thus confirming the presence of the water ligand in the mutant.

How photosynthetic reaction centers control oxidation power in chlorophyll pairs P680, P700, and P870

At the heart of photosynthetic reaction centers (RCs) are pairs of chlorophyll a (Chla), P700 in photosystem I (PSI) and P680 in photosystem II (PSII) of cyanobacteria, algae, or plants, and a pair of bacteriochlorophyll a (BChla), P870 in purple bacterial RCs (PbRCs). These pairs differ greatly in their redox potentials for one-electron oxidation, E(m). For P680, E(m) is 1,100-1,200 mV, but for P700 and P870, E(m) is only 500 mV. Calculations with the linearized Poisson-Boltzmann equation reproduce these measured E(m) differences successfully. Analyzing the origin for these differences, we found as major factors in PSII the unique Mn(4)Ca cluster (relative to PSI and PbRC), the position of P680 close to the luminal edge of transmembrane alpha-helix d (relative to PSI), local variations in the cd loop (relative to PbRC), and the intrinsically higher E(m) of Chla compared with BChla (relative to PbRC).

Function of redox-active tyrosine in photosystem II

Water oxidation at photosystem II Mn-cluster is mediated by the redox-active tyrosine Y(Z). We calculated the redox potential (E(m)) of Y(Z) and its symmetrical counterpart Y(D), by solving the linearized Poisson-Boltzmann equation. The calculated E(m)(Y( )/Y(-)) were +926 mV/+694 mV for Y(Z)/Y(D) with the Mn-cluster in S2 state. Together with the asymmetric position of the Mn-cluster relative to Y(Z/D), differences in H-bond network between Y(Z) (Y(Z)/D1-His(190)/D1-Asn(298)) and Y(D) (Y(D)/D2-His(189)/D2-Arg(294)/CP47-Glu(364)) are crucial for E(m)(Y(Z/D)). When D1-His(190) is protonated, corresponding to a thermally activated state, the calculated E(m)(Y(Z)) was +1216 mV, which is as high as the E(m) for P(D1/D2). We observed deprotonation at CP43-Arg(357) upon S-state transition, which may suggest its involvement in the proton exit pathway. E(m)(Y(D)) was affected by formation of P(D2)(+) (but not P(D1)(+)) and sensitive to the protonation state of D2-Arg(180). This points to an electrostatic link between Y(D) and P(D2).

Redox potentials of chlorophylls in the photosystem II reaction center

Water oxidation generating atmospheric oxygen occurs in photosystem II (PSII), a large protein-pigment complex located in the thylakoid membrane. The recent crystal structures at 3.2 and 3.5 A resolutions provide novel details on amino acid side chains, especially in the D1/D2 subunits. We calculated the redox potentials for one-electron oxidation of the chlorophyll a (Chla) molecules in PSII, considering the protein environment in atomic detail. The calculated redox potentials for the dimer Chla (P(D1/D2)) and accessory Chla (Chl(D1/D2)) were 1.11-1.30 V relative to the normal hydrogen electrode at pH 7, which is high enough for water oxidation. The D1/D2 proteins and their cofactors contribute approximately 390 mV to the enormous upshift of 470 mV compared to the redox potential of monomeric Chla in dimethylformamide. The other subunits are responsible for the remaining 80 mV. The high redox potentials of the two accessory Chla Chl(D1/D2) suggests that they also participate in the charge separation process.

Influence of the protein environment on the properties of a tyrosyl radical in reaction centers from Rhodobacter sphaeroides

The influence of the local environment on the formation of a tyrosyl radical was investigated in modified photosynthetic reaction centers from Rhodobacter sphaeroides. The reaction centers contain a tyrosine residue placed approximately 10 A from a highly oxidizing bacteriochlorophyll dimer. Measurements by both optical and electron paramagnetic resonance spectroscopy revealed spectral features that are assigned as arising primarily from an oxidized bacteriochlorophyll dimer at low pH values and from a tyrosyl radical at high pH values, with a well-defined transition that occurred with a pK(a) of 6.9. A model based on the wild-type structure indicated that the Tyr at M164 is likely to form a hydrogen bond with His M193 and to interact weakly with Glu M173. Substitution of Tyr or Glu for His at M193 increased the pK(a) for the transition from 6.9 to 8.9, while substitution of Gln for His M193 resulted in a higher pK(a) value. Substitution of Glu M173 with Gln resulted in loss of the partial formation of the tyrosyl that occurs in the other mutants at low pH values. The results are interpreted in terms of the ability of the residues to act as proton acceptors for the oxidized tyrosine, with the pK(a) values reflecting those of either the putative proton acceptor or the tyrosine, in accord with general models of amino acid radicals.

Functional analysis of combinatorial mutants with changes in the C-terminus of the CD loop of the D2 protein in photosystem II of Synechocystis sp. PCC 6803

Photosystem II properties were investigated in a set of combinatorial mutants containing changes in the C-terminal end of the CD lumenal loop (Gly187-Asn194) in the D2 protein of Synechocystis sp. PCC 6803. Initial screening of variable fluorescence (F(v)) induction and decay in the presence of DCMU showed that all but one of the combinatorial strains tested had an increased rate of Q(A)(-) reoxidation. Two strains showed an increase in the amplitude of constant fluorescence (F(o)). Examination of the primary sequence of the combinatorial strains combined with results obtained from analysis of site-directed mutants suggested that alterations in residue 191 of D2 increased the rate of charge recombination. Indeed, reintroduction of Trp191, the residue present in wild type, slowed the Q(A)(-) reoxidation rate in the presence of DCMU by 2-3-fold. However, the nature of other residues, in particular at codon 192, was also important in determining charge recombination rates. The increase in F(o) yield was due to an increased fluorescence lifetime of open reaction centers in intact cells and may reflect a decreased excitation trapping rate in the reaction center. This change was reversed by reintroduction of Trp191 even though a mutant lacking just Trp191 was normal in this respect. Trapping efficiency therefore was decreased only when multiple changes were present at the same time. We interpret Trp191 and neighboring residues to influence the midpoint redox potential of P680/P680(+) and in certain sequence contexts to affect the energy trapping efficiency by P680. The stability or environment of Y(D)(ox) was essentially unaffected in the mutants. Interestingly, many combinatorial mutants displayed an increased requirement for chloride for photoautotrophic growth, and two mutants, C8-10 and C8-23, also required more calcium. This indicates that this CD loop region of D2 not only affects properties of P680 but also affects properties of the oxygen-evolving complex.

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.

Photosynthetic water oxidation: towards a mechanism

This mini-review outlines the current theories on the mechanism of electron transfer from water to P680, the location and structure of the water oxidising complex and the role of the manganese cluster. We discuss how our data fit in with current theories and put forward our ideas on the location and mechanism of water oxidation.

Mutations in the CD-loop region of the D2 protein in Synechocystis sp. PCC 6803 modify charge recombination pathways in photosystem II in vivo

The lumenal CD-loop region of the D2 protein of photosystem II contains residues that interact with the primary electron donor P680 and the redox active tyrosyl residue Y(D). Photosystem II properties were studied in a number of photoautotrophic mutants of Synechocystis sp. PCC 6803, most of which carried combinatorial mutations in residues 164-170, 179-186, or 187-194 of the D2 protein. To facilitate characterization of photosystem II properties in the mutants, the CD-loop mutations were introduced into a photosystem I-less background. According to variable fluorescence decay measurements in DCMU-treated cells, charge recombination of Q(A)(-) with the donor side was faster in the majority of mutants (t(1/2) = 45-140 ms) than in the control (t(1/2) = 180 ms). However, in one mutant (named C7-3), the decay of Q(A)(-) was 2 times slower than in the control (t(1/2) = 360 ms). The decay half-time of each mutant correlated with the yield of the Q-band of thermoluminescence (TL) emitted due to S(2)Q(A)(-) charge recombination. The C7-3 mutant had the highest TL intensity, whereas no Q-band was detected in the mutants with fast Q(A)(-) decay (t(1/2) = 45-50 ms). The correlated changes in the rate of recombination and in TL yield in these strains suggest the existence of a nonradiative pathway of charge recombination between Q(A)(-) and the donor side. This may involve direct electron transfer from Q(A)(-) to P680(+) in a way not leading to formation of excited chlorophyll. Many mutations in the CD-loop appear to increase the equilibrium P680(+) concentration during the lifetime of the S(2)Q(A)(-) state, for example, by making the midpoint potential of the P680(+)/P680 redox couple more negative. The nonradiative charge recombination pathway involves a low activation energy and is less temperature-dependent than the formation of excited P680 that leads to TL emission. Therefore, during the TL measurements in these mutants, the S(2)Q(A)(-) state can recombine nonradiatively before temperatures are reached at which radiative charge recombination becomes feasible. The results presented here highlight the presence of two charge recombination pathways and the importance of the CD-loop of the D2 protein in determination of the energy gap between the P680(+)S(1) and P680S(2) states.

Probing the CD lumenal loop region of the D2 protein of photosystem II in Synechocystis sp. strain PCC 6803 by combinatorial mutagenesis

The CD lumenal loop region of the photosystem II reaction center protein D2 contains residues involved in oxygen evolution. Since detailed structural information about this region is unavailable, an M13-based combinatorial mutagenesis approach was used to investigate structure-function relationships in this vital region of D2 in Synechocystis sp. strain PCC 6803. The CD loop coding region contains close to 100 nucleotides, and for effective mutagenesis, it was subdivided into four regions of seven to eight codons. A gain-of-function selection protocol was employed such that all mutants that were selected contained a functional D2 protein. In this way, conservation patterns of residues along with numbers and types of amino acid substitutions accommodated at each position for each set of mutants would indicate which residues in the CD loop may play important structural and functional roles. Results of this study have substantiated the importance of residues previously studied by site-directed mutagenesis such as Arg180 and His189 and have identified other previously unremarkable residues in the CD loop (such as Ser166, Phe169, and Ala170) that cannot be replaced by many other residues. In addition, the pliability of the CD loop was further tested using deletion and D1-D2 substitution constructs in M13. This showed that the length of the loop was important to its function, and in two cases, D2 could accommodate homologous sequences from D1, which forms a heterodimer with D2 in photosystem II, but not the other way around. This study of the CD loop in D2 provides valuable clues regarding the structural and functional requirements of the region.

Tryptophan at position 181 of the D2 protein of photosystem II confers quenching of variable fluorescence of chlorophyll: implications for the mechanism of energy-dependent quenching

The lumenal CD loop region of the D2 protein of photosystem II contains residues that interact with a reaction center chlorophyll and the redox-active Tyr(D). Using combinatorial mutagenesis, photoautotrophic mutants of Synechocystis sp. PCC 6803 have been generated with multiple amino acid changes in this region. The CD loop mutations were transferred into a photosystem I-less Synechocystis strain to facilitate characterization of photosystem II properties in the mutants. Most of the combinatorial photosystem I-less mutants obtained had a high yield of variable fluorescence, F(V). However, in three mutants, which shared a replacement of Phe181 by Trp, the F(V) yield was dramatically reduced although a high rate of oxygen evolution was maintained. A site-directed F181W D2 mutant shared similar properties. Picosecond time-resolved fluorescence measurements revealed that in the combinatorial F181W mutants the fluorescence lifetimes in closed and open photosystem II centers were essentially identical and were similar to the fluorescence lifetime in open centers of the control strain. These results are explained by quenching of variable fluorescence in the mutants by charge separation between Trp181 and excited reaction center chlorophyll. This reaction competes efficiently with fluorescence and nonradiative decay in closed photosystem II centers, where the lifetime of the excitation in the chlorophyll antenna is long. Thermodynamic considerations favor the formation of oxidized tryptophan and reduced chlorophyll in the quenching reaction, presumably followed by charge recombination. A possible role of tryptophan-chlorophyll charge separation in the mechanism of energy-dependent quenching of excitations in photosynthesis is discussed.

Photosystem II of green plants: on the possible role of retarded protonic relaxation in water oxidation1

Photosystem II (PSII) of green plants and cyanobacteria uses energy of light to oxidize water and to produce oxygen. The available estimates of the oxidizing potential of P680+, the primary donor of PSII, yield value of about 1.15 V. Two main factors are suggested to add up and engender this high oxidizing potential, namely: (1) the electrostatic influence dominated by Arg-181 of the D2 subunit which elevates the oxidizing potential of P680+ up to 1 V, some 0.1 V above the Em value of a hydrogen-bonded chlorophyll a; and (2) the dynamic component of 0.10-0.15 V due to the experimentally demonstrated retarded protonic relaxation at the P680 site.

Mobility of the primary electron-accepting plastoquinone QA of photosystem II in a Synechocystis sp. PCC 6803 strain carrying mutations in the D2 protein

Upon introduction of random mutations in a region of the psbDI gene that encodes the D2 protein in the cyanobacterium Synechocystis sp. PCC 6803, an obligate photoheterotrophic mutant was isolated that contained three mutations: V247M, A249T, and M329I. This mutant evolved oxygen in the absence of added electron acceptors, but oxygen evolution was inhibited by micromolar concentrations of several artificial quinones. Complementation analysis showed that the V247M and/or A249T mutations were responsible for this phenotype. Using fluorescence induction and decay measurements, the site of inhibition by the quinones was found to be at the level of the primary electron-accepting quinone in photosystem II, QA. Duroquinone inhibited by blocking reduction of QA, and in the presence of other quinones such as 2,5-dichloro-p-benzoquinone, 2, 5-dimethyl-p-benzoquinone, and p-benzoquinone, QA could be reduced but could not efficiently transfer an electron to QB. To distinguish the effects of the V247M and A249T mutations, single mutants were created. V247M was photoautotrophic and had an essentially normal phenotype. The A249T mutant, although photoautotrophic, was affected by artificial quinones, but less than the mutant carrying both the V247M and A249T changes. The results indicate a decreased plastoquinone affinity at the QA site in the strains carrying a A249T mutation, such that after dark-adaptation a significant percentage of the QA sites is empty or is occupied by an artificial quinone. In light, the percentage of photosystem II centers with plastoquinone bound at the QA site appears to increase, which may be due in part to an increased affinity of the semiquinone versus that of the quinone at the QA site.