Energy transfer and quantum yield in Photosystem II

The photoreduction and dark reoxidation of Q_α and Q_β, the primary electron acceptors of Photosystems (PS) IIα and IIβ, respectively, in the presence of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea (DCMU) were studied in tobacco chloroplasts by means of fluorescence and absorbance measurements. The magnitude of a correction for an absorbance change by the oxidizing side of PS II needed in our previous study of the quantum yield of Q reduction (Biochim. Biophys. Acta 635 (1981), 111–120) has been determined. The absorbance change occurs in PS IIα mainly. The maximum fluorescence yield was found to be the same as in the mutant Su/su, which has a 3-fold higher reaction center concentration and a lower PS IIα to PS IIβ ratio. The kinetics of the light-induced fluorescence increase were measured after various pretreatments and the corresponding kinetics of the integrated fluorescence deficit were analyzed into their α and β components. From the results the contribution to the minimum fluorescence level, the degree of energy transfer between units, and the quantum efficiency of Q reduction were calculated for both types of PS II. This led to the following conclusions. The absence of energy between PS IIβ antennae is confirmed. Fluorescence quenching in PS IIα was adequately described by the matrix model, except for a decrease in the energy transfer between units during photoreduction of Q_α, possibly due to the formation of ‘islets’ of closed centers. PS II reaction centers in which Q is reduced do not significantly quench fluorescence. The ratio of variable to maximum fluorescence, 0.77 in PS IIα and 0.92 in PS IIβ, multiplied by the fraction of Q remaining in the reduced state after one saturating flash, 0.88 in PS IIα and greater than 0.95 in PS IIβ, leads to a net quantum efficiency of Q reduction in the presence of DCMU and NH₂OH of 0.68 in PS IIα and about 0.90 in PS IIβ. These values are in good agreement with the measured overall quantum efficiency of Q reduction.     

Kinetics of EPR signal IIvf in chloroplast Photosystem II

The risetime of EPR signal II_vf (S II_vf) has been measured in oxygen-evolving Photosystem II particles from spinach chloroplasts at pH 6.0. The EPR signal shows an instrument-limited rise upon induction ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{? 3 μ}\text{s}$). These data are consistent with a model where the species Z responsible for S II_vf is the immediate electron donor to P-680⁺ in spinach chloroplasts. A new, faster decay component of S II_vf has also been detected in these experiments.     

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

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

Photosystem I photochemistry at low temperature. Heterogeneity in pathways for electron transfer to the secondary acceptors and for recombination processes

Electron transport has been studied by flash absorption and EPR spectroscopies at 10–30 K in Photosystem I particles prepared with digitonin under different redox conditions. In the presence of ascorbate, an irreversible charge separation is progressively induced at 10 K between P-700 and iron-sulfur center A by successive laser flashes, up to a maximum which corresponds to about two-thirds of the reaction centers. In these centers, heterogeneity of the rate for center A reduction is also shown. In the other third of reaction centers, the charge separation is reversible and relaxes with a t_1/2 ≈ 120 μs. When the iron-sulfur centers A and B are prereduced, the 120 μs relaxation becomes the dominant process (70–80% of the reaction centers), while a slow component (t_1/2 = 50–400 ms) reflecting the recombination between P-700⁺ and center X⁻ occurs in a minority of reaction centers (10–15%). Flash absorption and EPR experiments show that the partner of P-700⁺ in the 120 μs recombination is neither X nor a chlorophyll but more probably the acceptor A⁻₁ as defined by Bonnerjea and Evans (Bonnerjea, J. and Evans, M.C.W. (1982) FEBS Lett. 148, 313–316). The role of center X in low-temperature electron flow is also discussed.     

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.     

Stimulation by manganese and other divalent cations of the electron donation reactions of Photosystem II

Using inside-out thylakoid membranes, it has been shown that the oxidation of water and associated reduction of dichlorophenol indophenol is partially inhibited by low concentrations of cation chelators. This inhibition correlates with a removal of two manganese ions per Photosystem II reaction centre. The chelator-induced inhibition was completely reversed by the addition of low levels of Mn²⁺ ($\text{C}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 20 μ}\text{M}$) and higher levels of Mg²⁺ and Ca²⁺ ($\text{C}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 1}\text{mM}$). Other cations were not effective, indicating that the ability to overcome the inhibition did not involve a general electrostatic screening process. The degree of inhibition by chelators was greater at lower light intensities and after treatment with glutaraldehyde. In the presence of glutaraldehyde the stimulatory effect of Mn²⁺ was lost, while pretreatment with Mn²⁺ prevented the glutaraldehyde effect. These results are discussed in terms of conformational changes of the electron donation chains involving cation- (preferentially Mn-) dependent coupling between the oxygen evolving and reaction-centre complexes of Photosystem II.     

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

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

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.     

Primary and secondary electron donors in Photosystem II of chloroplasts. Rates of electron transfer and location in the membrane

Absorption changes at 820 or 515 nm after a short laser flash were studied comparatively in untreated chloroplasts and in chloroplasts in which oxygen evolution is inhibited.In chloroplasts pre-treated with Tris, the primary donor of Photosystem II (P-680) is oxidized by the flash, as observed by an absorption increase at 820 nm. After the first flash it is re-reduced in a biphasic manner with half-times of 6 μs (major phase) and 22 μs. After the second flash, the 6 μs phase is nearly absent and P-680⁺ decays with half-times of 130 μs (major phase) and 22 μs. Exogenous electron donors (MnCl₂ or reduced phenylenediamine) have no direct influence on the kinetics of P-680⁺.In untreated chloroplasts the 6 and 22 μs phases are of very small amplitude, either at the 1st, 2nd or 3rd flash given after dark-adaptation. They are observed, however, after incubation with 10 mM hydroxylamine.These results are interpreted in terms of multiple pathways for the reduction of P-680⁺: a rapid reduction (<1 μs) by the physiological donor D₁; a slower reduction (6 and 22 μs) by donor D′₁, operative when O₂ evolution is inhibited; a back-reaction (130 μs) when D′₁ is oxidized by the pre-illumination in inhibited chloroplasts. In Tris-treated chloroplasts the donor system to P-680⁺ has the capacity to deliver only one electron.The absorption change at 515 nm (electrochromic absorption shift) has been measured in parallel. It is shown that the change linked to Photosystem II activity has nearly the same magnitude in untreated chloroplasts or in chloroplasts treated with hydroxylamine or with Tris (first and subsequent flashes). Thus we conclude that all the donors (P-680, D₁, D′₁) are located at the internal side of the thylakoid membrane.     

The dependence of reaction center and antenna triplets on the redox state of Photosystem I

The formation of chlorophyll triplet states during illumination of Photosystem I reaction center samples depends upon the redox state of P-700, X and ferredoxin Centers A and B. When the reaction centers are in the states P-700⁺A₁XFd_BFd^?_A and P-700 A₁XFd^?_BFd^?_A prior to illumination, we observe electron paramagnetic resonance (EPR) spectra from a triplet species which has zero-field splitting parameters (|D| and |E|) larger than those of either the chlorophyll a or chlorophyll b monomer triplet, and a polarization which results from population of the triplet spin sublevels by an intersystem crossing mechanism. We interpret this triplet as arising from photoexcited chlorophyll antenna species associated with reaction centers in the states P-700⁺Fd^?_A and P-700⁺X^?, respectively, which undergo de-excitation via intersystem crossing. When the reaction centers are in the states P-700A₁XFd^?_BFd^?_A and P-700A₁X^?Fd^?_BFd^?_A prior to illumination, we observe a triplet EPR signal with a polarization which results from population of the triplet spin sublevels by radical pair recombination, and which has a |D| value similar to that of chlorophyll a monomer. We interpret this triplet (the radical pair-polarized triplet) as arising from ³P-700 which has been populated by the process $\text{P-700}{}^{\mathrm{+}}\text{A}{}^{\mathrm{?}}{}_1\text{→}{}^3\text{P-700}\text{A}{}_1$. We observe both the radical pair-polarized triplet and the chlorophyll antenna triplet when the reaction centers are in the state P-700 A₁XFd^?_BFd^?_A, presumably because the processes P-700⁺A^?₁X → P-700⁺A₁X^? and $\text{P-700}{}^{\mathrm{+}}\text{A}{}^{\mathrm{?}}{}_1\text{X}\text{→}{}^3\text{P-700}\text{A}{}_1\text{X}$ have similar rate constants when Centers A and B are reduced, i.e., the forward electron transfer time from A^?₁ to X is apparently much slower in the redox state P-700 A₁XFd^?_BFd^?_A than it is in state P-700 A₁XFd_BFd_A. The amplitude of the radical pair-polarized triplet EPR signal does not decrease in the presence of a 13.5-G-wide EPR signal centered at g 2.0 which was recorded in the dark prior to triplet measurements in samples previously frozen under intense illumination. This g 2.0 signal, which has been attributed to phototrapped A^?₁ (Heathcote, P., Timofeev, K.N. and Evans, M.C.W. (1979) FEBS Lett. 101, 105–109), corresponds to as many as 12 spins per P-700 and can be photogenerated during freezing without causing any apparent attenuation of the radical pair-polarized triplet amplitude. We conclude that species other than A^?₁ contribute to the g 2.0 signal.     

The effects of mono- and divalent salts on the O2-evolution activity and low temperature multiline EPR spectrum of Photosystem II preparations from spinach

The ability of salts to inhibit the O₂-evolution activity of PS II preparations is shown to parallel closely the Hofmeister series, suggesting that inhibition is related to the solubility of the 16, 24 and 33 kDa proteins in these salt solutions. An examination of the effect of salt inactivation on the low temperature multiline EPR signal indicates that the release of either the 16 and 24 kDa proteins, or additionally the 33 kDa protein blocks or greatly reduces the efficiency of the advancement of the water-splitting complex to the S₂-state; under some conditions, this inhibition is reversible.     

Thermoluminescence as a probe of Photosystem II photochemistry. The origin of the flash-induced glow peaks

A single flash given at − 15°C to chloroplasts results in charge separation in Photosystem II to form a stable state which, upon warming, recombines giving rise to luminescence. This recombination occurs at 25°C in untreated chloroplasts but is shifted to 0°C in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea or weak concentrations of a reducing agent. The luminescence at 0°C is attributed to recombination of the S₂Q⁻_A state while that at 25°C is attributed to recombination of S₂Q_AQ⁻_B (and S₃Q_AQ⁻_B upon further flash illumination). The identification of the thermoluminescence at 25°C is based upon the following experimental evidence: (1) illumination of chloroplasts in the presence of methyl viologen with 710 nm light before and after flash illumination has no effect on the extent or temperature of the thermoluminescence. This is taken as evidence that the plastoquinone pool is not involved in the recombination reaction. (2) Calculations of the extent of thermoluminescence expected after a number of flashes, assuming that S₂Q_AQ⁻_B and S₃Q_AQ⁻_B are the thermoluminescent reactants, give a good fit to the experimental results. (3) The effect of continuous illumination at 77 K (i.e., donation from cytochrome b-559 to Q_A and thence to Q_B or Q⁻_B) results in predictable changes in the extent of flash-induced thermoluminescence.     

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

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

Investigation of the apparent inefficiency of the coupling between Photosystem II electron transfer and ATP formation

The maximum phosphorylation efficiency achieved with synchronous turnovers of Photosystem II (PS II) in spinach chloroplast lamellae is 0.3 molecules of ATP per pair of electrons transferred. This is the same as the efficiency observed for PS II operating alone in continuous light and would seem to indicate less than 50% coupling efficiency. Flash-induced ATP synthesis associated with both photosystems acting in unison closely approaches twice the flash-induced ATP synthesis associated with the Photosystem-I-dependent oxidation of duroquinol (itself 0.6) and comes close to equalling the highest efficiency observed in steady-state PS I + PS II electron transport. The anomalously low coupling efficiency seen when PS II is operating alone can be overcome by a ΔpH of two units imposed before flash illumination, or by a prior flash series involving the entire electron transfer chain. In contrast, prior electron transport through PS II alone is only slightly effective in enhancing the coupling efficiency of subsequent PS II turnovers. (It should be noted that in all cases where supplementary energy was provided, either by a proton gradient or by prior illumination, this supplementary energy was always below the energetic threshold for phosphorylation. Furthermore, the enhancement of PS II coupling efficiency by supplementary energy persisted even after a large number of subsequent PS II-inducing flashes). The efficiency of flash-induced ATP synthesis associated with whole-chain electron transfer or with PS-I-dependent duroquinol oxidation is also enhanced by the supplementary energy, but only during the first few inefficient flashes, suggesting that in this case the supplementary energy may simply be contributing to the initial build-up of an energetic threshold for ATP synthesis. This cannot be the case when the same supplementary energy contributes to the efficiency of the PS II reaction, since the enhancement then persists for a long time and contributes to an essentially constant flash yield of ATP. Our results imply that during electron transfer involving both photosystems, PS II participates in generating about half of the total ATP, whereas it operates inefficiently only when operating alone. Since hydrogen ions produced by PS I are able to raise the efficiency of subsequent PS-II-dependent phosphorylation, at least some cooperation between the two photosystems takes place and this suggests some donation of protons from PS I to PS II. However, the inability of PS II alone to achieve high efficiency, even with prolonged pre-illumination, would seem to indicate some functional distinction of protons from the two photosystems.     

Dynamics of electron transfer in photosystem II

Photosystem II, being a constituent of light driven photosynthetic apparatus, is a highly organized pigment-protein-lipid complex. The arrangement of PSII active redox cofactors insures efficiency of electron transfer within it. Donation of electrons extracted from water by the oxygen evolving complex to plastoquinones requires an additional activation energy. In this paper we present theoretical discussion of the anharmonic fluctuations of the protein-lipid matrix of PSII and an experimental evidence showing that the fluctuations are responsible for coupling of its donor and acceptor side. We argue that the fast collective motions liberated at temperatures higher that 200 K are crucial for the two final steps of the water splitting cycle and that one can distinguish three different dynamic regimes of PSII action which are controlled by the timescales of forward electron transfer, which vary with temperature. The three regimes of the dynamical behavior are related to different spatial domains of PSII.     

The Effect of Cadmium on Photosystem II in Spinach Chloroplasts

Cadmium ions, as an environmental pollution factor, significantly inhibited the photosynthesis especially, photosystem Ⅱ activity in isolated spinach chloroplasts. The presence of 5 mmol/l Cd2+ inhibited the O2-evolution to 53%. Cd2+ reduced the activity of photoreduction of DCIP and the variable fluorescence of chloroplasts and PSⅡ preparation. The inhibited DCIP photoreduction activity could only be restored slightly by the addition of an artificial electron donor of PSII, DPC, and the inhibited variable fluorescence could not be obviously recovered by the addition of NH2OH, another artificial electron donor of PSⅡ. It is considered that, besides the oxidizing side of PSI1, Cd2+ could also inhibit directly the PSⅡ reaction center. The inhibitory effect of Cd2+ on the whole chain electron transport (H2O→MV) was more serious than on O2-evolution (H2O→DCMU). It is suggested that the oxidizing side of PSⅡ is not the only site for Cd2+ action. There may be another site inhibited by Cd2+ in the electron transport chain between PSⅠ and PSⅡ.     

Energy transfers from Photosystem II to Photosystem I in Cryptomonas rufescens (Cryptophyceae)

In Cryptomonas rufescens (Cryptophyceae), phycoerythrin located in the thylakoid lumen is the major accessory pigment. Oxygen action spectra prove phycoerythrin to be efficient in trapping light energy.The fluorescence excitation spectra at ?196°C obtained by the method of Butler and Kitajima (Butler, W.L. and Kitajima, M. (1975) Biochim. Biophys. Acta 396, 72–85) indicate that like in Rhodophycease, chlorophyll a is the exclusive light-harvesting pigment for Photosystem I.For Photosystem II we can observe two types of antennae: (1) a light-harvesting chlorophyll complex connected to Photosystem II reaction centers, which transfers excitation energy to Photosystem I reaction centers when all the Photosystem II traps are closed. (2) A light-harvesting phycoerythrin complex, which transfers excitation energy exclusively to the Photosystem II reaction complexes responsible for fluorescence at 690 nm.We conclude that in Cryptophyceae, phycoerythrin is an efficient light-harvesting pigment, organized as an antenna connected to Photosystem II centers, antenna situated in the lumen of the thylakoid. However, we cannot afford to exclude that a few parts of phycobilin pigments could be connected to inactive chlorophylls fluorescing at 690 nm.     

Evidence that the low-potential (−700 mV) electron acceptor (X) in Photosystem I has two iron-sulphur centres

The Photosystem I reaction centre contains two groups of iron-sulphur centres: Fe-S_A and Fe-S_B with redox potentials between ?510 and ?590 mV, and Fe-S_X with redox potential about ?700 mV. Spin quantitation (Heathcote, P., Williams-Smith, D.L. and Evans, M.C.W. (1978) Biochem. J. 170, 373–378) and Mössbauer spectroscopy (Evans, E.H., Dickson, D.P.E., Johnson, C.E., Rush, J.D. and Evans, M.C.W. (1981) Eur. J. Biochem. 118, 81–84) did not show unequivocally whether Fe-S_X has one or two centres. Experiments are described which support the proposal that Fe-S_X has two centres. Fe-S_X can be photoreduced irreversibly by 210 K illumination of dithionite-reduced samples or reversibly by 7.5 K illumination of these samples. The amplitude of the Fe-S_X signal reversibly induced by illumination at 7.5 K is never more than 50% of the amplitude of the signal when Fe-S_X is prereduced by room temperature illumination or by 210 K illumination. Approx. half of the Fe-S_X is rapidly reduced by 210 K illumination, the remainder more slowly. The extent of reversible Fe-S_X reduction and P-700 photooxidation is little affected by the fast reduction of about half of the Fe-S_X. Subsequent reduction of the remaining Fe-S_X is paralleled by loss of the reversible photoreaction.     

Sulfhydryl reagents inhibit electron transport in Photosystem II of spinach chloroplasts

A 120 min incubation period with sulfhydryl reagents, such as p-chloromercuribenzoic acid, shows greater than 50% loss of electron-transport activity in Photosystem (PS) II of spinach chloroplasts. Since p-chloromercuriphenylsulfonic acid, a nonpenetrating sulfhydryl reagent, and 4,4′-dithiopyridine, a bifunctional sulfhydryl reagent, show greater inhibition of 3-(3,4-dichlorophenyl)-1,1-dimethylurea-insensitive silicomolybdate reduction than of dibromothymoquinone-insensitive indophenol reduction, it is postulated that two different sulfhydryl reagent-sensitive sites are involved in the PS II electron-transport chain of spinach chloroplasts.     

Identity of the Photosystem II reaction center polypeptide

A Photosystem-II (PS-II)-enriched chloroplast submembrane fraction has been subjected to non-denaturing gel-electrophoresis. Two chlorophyll a (Chl a)-binding proteins associated with the core complex were isolated and spectrally characterized. The Chl protein with apparent apoprotein mass of 47 kDa (CP47) displayed a 695 nm fluorescence emission maximum (77 K) and light-induced absorption characteristics indicating the presence of the reaction center Chl, P-680, and its primary electron acceptor, pheophytin. A Chl protein of apparent apoprotein mass of 43 kDa (CP43) displayed a fluorescence emission maximum at 685 nm. We conclude that CP43 serves as an antenna Chl protein and the PS II reaction center is located in CP47.