Search

Matrix effects on long-range electron transfer were studied in cyanobacterial Photosystem I (PS I) complexes, embedded into trehalose glasses at different hydration levels. W-band EPR studies demonstrated, via nitroxide spin probes, structural homogeneity of the dry PS I-trehalose matrix and no alteration of cofactors' distance and relative orientation under temperature and matrix variation. In dry trehalose glasses at room temperature (RT), PS I was stable for months. Flash-induced charge recombination kinetics were examined by high-field time-resolved EPR and optical spectroscopies. The kinetics in hydrated PS I-trehalose glasses mostly reflected the reduction of the photooxidized primary donor P700•+ by the reduced terminal iron-sulfur clusters. Upon dehydration, the P700•+ decay accelerated and became more distributed. Continuous distributions of lifetimes τ were extracted from the kinetics by two numerical approaches: a maximum entropy method (MemExp program) and a constrained regularization method (CONTIN program). Both analyses revealed that upon dehydration the contribution of the two slowest components (lifetimes τ ~ 300 ms and ~ 60 ms), attributed to P700•+[FA/FB] − recombination, decreased in parallel with the increase of the fastest component (τ ~ 150 μs), and of additional distributed phases with intermediate lifetimes. Dehydration at RT mimicked the effects of freezing water-glycerol PS I systems, suggesting an impairment of PS I protein dynamics in the dry trehalose glass. Similar effects were observed previously in bacterial reaction centers. The work presented for PS I provides new insights into the crucial issue of protein-matrix interactions for protein functionality as controlled by hydrogen-bond networks of the hydration shell.

Chlamydomonas reinhardtii is a photoautotrophic green alga, which can be grown mixotrophically in acetate-supplemented media (Tris–acetate–phosphate). We show that acetate has a direct effect on photosystem II (PSII). As a consequence, Tris–acetate–phosphate-grown mixotrophic C. reinhardtii cultures are less susceptible to photoinhibition than photoautotrophic cultures when subjected to high light. Spin-trapping electron paramagnetic resonance spectroscopy showed that thylakoids from mixotrophic C. reinhardtii produced less 1 O 2 than those from photoautotrophic cultures. The same was observed in vivo by measuring DanePy oxalate fluorescence quenching. Photoinhibition can be induced by the production of 1 O 2 originating from charge recombination events in photosystem II, which are governed by the midpoint potentials ( E m ) of the quinone electron acceptors. Thermoluminescence indicated that the E m of the primary quinone acceptor (Q A /Q A − ) of mixotrophic cells was stabilised while the E m of the secondary quinone acceptor (Q B /Q B − ) was destabilised, therefore favouring direct non-radiative charge recombination events that do not lead to 1 O 2 production. Acetate treatment of photosystem II-enriched membrane fragments from spinach led to the same thermoluminescence shifts as observed in C. reinhardtii , showing that acetate exhibits a direct effect on photosystem II independent from the metabolic state of a cell. A change in the environment of the non-heme iron of acetate-treated photosystem II particles was detected by low temperature electron paramagnetic resonance spectroscopy. We hypothesise that acetate replaces the bicarbonate associated to the non-heme iron and changes the environment of Q A and Q B affecting photosystem II charge recombination events and photoinhibition.

Thermoluminescence of Photosystem II particles isolated from pea chloroplasts using digitonin and Triton X-100 was measured after 1 min illumination at a certain temperature (T(ex)) followed by illumination during cooling (40 Cdeg/min) to a lower temperature. Glow curves of the particles are characteristic of the photosynthetic oxygen-evolving material studied earlier. Complete (more than 95%) removal of Mn from the Photosystem II particles abolishes thermoluminescence bands around 0° C, related to the oxygen-evolving system, but the thermoluminescence bands peaking around -30°C (TL(-30)), -55°C (TL_ (-55)) and between-68 and -85° C, depending on Tex(TLv), remain unaltered. The bands are characterized by different dependence on T,x. The TL(-30), TL(-55) and TL v bands can also be observed in the glow curve of isolated pea and spinach chloroplasts. Re-addition of MnCI (2) (2 μM, corresponding to nearly 4 Mn atoms per reaction center of Photosystem II) to the Mn-depleted particles does not reactivate the thermoluminescence bands around 0° C. However, it does lead to suppression of TL(-30) accompanied by parallel activation of TL(-55), revealing competition of the TL (-30) and TL(-55) for charges generated by the reaction center. These data, as well as the results on the effect of inhibitors and electron donors to Photosystem II, show that positive charges contributing to the TL(-30), TL (-55) and TL v thermoluminescence bands are located on secondary electron donors of Photosystem II which do not require Mn and are located closer to the reaction center than the Mn-containing, water-oxidizing enzyme.

Exposure of wild type (WT) and plastocyanin coding petE gene deficient mutant (ΔpetE) of Synechococcus cells to low iron growth conditions was accompanied by similar iron-stress induced blue-shift of the main red Chl a absorption peak and a gradual decrease of the Phc/Chl ratio, although ΔpetE mutant was more sensitive when exposed to iron deficient conditions. Despite comparable iron stress induced phenotypic changes, the inactivation of petE gene expression was accompanied with a significant reduction of the growth rates compared to WT cells. To examine the photosynthetic electron fluxes in vivo, far-red light induced P700 redox state transients at 820nm of WT and ΔpetE mutant cells grown under iron sufficient and iron deficient conditions were compared. The extent of the absorbance change (ΔA(820)/A(820)) used for quantitative estimation of photooxidizable P700(+) indicated a 2-fold lower level of P700(+) in ΔpetE compared to WT cells under control conditions. This was accompanied by a 2-fold slower re-reduction rate of P700(+) in the ΔpetE indicating a lower capacity for cyclic electron flow around PSI in the cells lacking plastocyanin. Thermoluminescence (TL) measurements did not reveal significant differences in PSII photochemistry between control WT and ΔpetE cells. However, exposure to iron stress induced a 4.5 times lower level of P700(+), 2-fold faster re-reduction rate of P700(+) and a temperature shift of the TL peak corresponding to S(2)/S(3)Q(B)(-) charge recombination in WT cells. In contrast, the iron-stressed ΔpetE mutant exhibited only a 40% decrease of P700(+) and no significant temperature shift in S(2)/S(3)Q(B)(-) charge recombination. The role of mobile electron carriers in modulating the photosynthetic electron fluxes and physiological acclimation of cyanobacteria to low iron conditions is discussed. This article is part of a Special Issue entitled: Photosynthesis Research for Sustainability: from Natural to Artificial.

Photosystem I of cyanobacteria contains different spectral pools of chlorophylls called red or long-wavelength chlorophylls that absorb at longer wavelengths than the primary electron donor P700. We measured the fluorescence spectra at the ensemble and the single-molecule level at low temperatures in the presence of oxidized and reduced P700. In accordance with the literature, it was observed that the fluorescence is quenched by P700+. However, the efficiency of the fluorescence quenching by oxidized P700+ was found to be extremely different for the various red states in PS I from different cyanobacteria. The emission of the longest-wavelength absorbing antenna state in PS I trimers from Thermosynechococcus elongatus (absorption maximum at 5 K: ≅ 719 nm; emission maximum at 5 K: ≅ 740 nm) was found to be strongly quenched by P700+ similar to the reddest state in PS I trimers from Arthrospira platensis emitting at 760 nm at 5 K. The fluorescence of these red states is diminished by more than a factor of 10 in the presence of oxidized P700. For the first time, the emission of the reddest states in A. platensis and T. elongatus has been monitored using single-molecule fluorescence techniques.

Photosystem I particles from Prochlorothrix hollandica were isolated from dodecylmaltoside solubilized thylakoid membranes on sucrose gradients in the presence of dodecylmaltoside. The particles were characterized by electron microscopy and image reconstruction techniques. The lowest, major green band in the gradient contained trimeric Photosystem I particles with features similar to Photosystem I from cyanobacteria. No evidence for an association of the chlorophyll a/b-binding antenna with Photosystem I was found. The trimeric association of Photosystem I appears to be a generally occurring aggregation mechanism in oxygenic prokaryotes.

Phycobilisomes (PBS) are the major photosynthetic antenna complexes in cyanobacteria and red algae. In the red microalga Galdieria sulphuraria, action spectra measured separately for photosynthetic activities of photosystem I (PSI) and photosystem II (PSII) demonstrate that PBS fraction attributed to PSI is more sensitive to stress conditions and upon nitrogen starvation disappears from the cell earlier than the fraction of PBS coupled to PSII. Preillumination of the cells by actinic far-red light primarily absorbed by PSI caused an increase in the amplitude of the PBS low-temperature fluorescence emission that was accompanied by the decrease in PBS region of the PSI 77 K fluorescence excitation spectrum. Under the same conditions, fluorescence excitation spectrum of PSII remained unchanged. The amplitude of P700 photooxidation in PBS-absorbed light at physiological temperature was found to match the fluorescence changes observed at 77 K. The far-red light adaptations were reversible within 2–5min. It is suggested that the short-term fluorescence alterations observed in far-red light are triggered by the redox state of P700 and correspond to the temporal detachment of the PBS antenna from the core complexes of PSI. Furthermore, the absence of any change in the 77 K fluorescence excitation cross-section of PSII suggests that light energy transfer from PBS to PSI in G. sulphuraria is direct and does not occur through PSII. Finally, a novel photoprotective role of PBS in red algae is discussed.

1. 1. In the presence of ≧ 3 mM divalent cations or ≧ 100 mM monovalent cations, weak 650-nm light, presumably containing an excess of Photosystem II quanta, caused substantial reduction of the electron carrier pool between the two photoacts. In low-salt media, most electron carriers were oxidized during red light. 2. 2. In the presence of low concentrations of carbonylcyanide m -chlorophenylhydrazone (CCCP) (0.3 μM) or antimycin A (40 μM) the pool remained oxidized even in the presence of adequate cation concentrations. 3. 3. The non-linear dependence of the O 2 -evolution rate upon the concentration of active Photosystem II trapping centers, which implies energy transfer between Photosystem II units, was observed only in the presence of sufficient cation. 4. 4. Enhancement of the rate of methyl viologen reduction in far-red light by red light was found to be a weak function of Mg 2+ concentration. 5. 5. With ferredoxin-NADP + as acceptor, enhancement of the rate of O 2 evolution in 650-nm light by far-red light was obtained only with added Mg 2+ . Furthermore, Mg 2+ addition markedly stimulated the quantum yields of NADP + reduction, independent of wavelength, with either water or ascorbate-reduced 2,6-dichlorophenolindophenol (DCIP) as the electron donor. A dual effect of cations in the ferredoxin-NADP + system is suggested. 6. 6. With methyl viologen or potassium ferricyanide as acceptor and water as donor, Mg 2+ did not affect the quantum yield in 650-nm light and slightly increased the yield at longer wavelengths. The quantum yield of the ascorbate-reduced DCIP-methyl viologen (Photosystem I) reaction was slightly decreased in 650-nm light and unaffected at long wavelengths. Our interpretation is that cation concentration affects the pigment distribution between Photosystems I and II.

Photosystem I (PS I) mediates light-induced electron transfer from P700 through a chlorophyll a, a quinone and a [4Fe-4S] iron-sulfur cluster F(X), located on the core subunits PsaA/B to iron-sulfur clusters F(A/B) on subunit PsaC. Structure function relations in the native and in the mutant (psaB-C565S/D566E) of the cysteine ligand of F(X) cluster were studied by X-ray absorption spectroscopy (EXAFS) and transient spectroscopy. The structure of F(X) was determined in PS I lacking clusters F(A/B) by interruption of the psaC2 gene of PS I in the cyanobacterium Synechocystis sp PCC 6803. PsaC-deficient mutant cells assembled the core subunits of PS I which mediated electron transfer mostly to the phylloquinone. EXAFS analysis of the iron resolved a [4Fe-4S] cluster in the native PsaC-deficient PS I. Each iron had 4 sulfur and 3 iron atoms in the first and second shells with average Fe-S and Fe-Fe distances of 2.27 A and 2.69 A, respectively. In the C565S/D566E serine mutant, one of the irons of the cluster was ligated to three oxygen atoms with Fe-O distance of 1.81 A. The possibility that the structural changes induced an increase in the reorganization energy that consequently decreased the rate of electron transfer from the phylloquinone to F(X) is discussed.

Absorbance difference spectroscopy and redox titrations have been applied to investigate the properties of photosystem I from the chlorophyll d containing cyanobacterium Acaryochloris marina. At room temperature, the (P740(+)-P740) and (F(A/B)(-)-F(A/B)) absorbance difference spectra were recorded in the range between 300 and 1000 nm while at cryogenic temperatures, (P740(+)A(1)(-)-P740A(1)) and ((3)P740-P740) absorbance difference spectra have been measured. Spectroscopic and kinetic evidence is presented that the cofactors involved in the electron transfer from the reduced secondary electron acceptor, phylloquinone (A(1)(-)), to the terminal electron acceptor and their structural arrangement are virtually identical to those of chlorophyll a containing photosystem I. The oxidation potential of the primary electron donor P740 of photosystem I has been reinvestigated. We find a midpoint potential of 450+/-10 mV in photosystem I-enriched membrane fractions as well as in thylakoids which is very similar to that found for P700 in chlorophyll a dominated organisms. In addition, the extinction difference coefficient for the oxidation of the primary donor has been determined and a value of 45,000+/-4000 M(-1) cm(-1) at 740 nm was obtained. Based on this value the ratio of P740 to chlorophyll is calculated to be 1 : to approximately 200 chlorophyll d in thylakoid membranes. The consequences of our findings for the energetics in photosystem I of A. marina are discussed as well as the pigment stoichiometry and spectral characteristics of P740.

A photosystem I (PSI)–fucoxanthin chlorophyll protein (FCP) complex with a chlorophyll a/P700 ratio of approximately 200:1 was isolated from the diatom Phaeodactylum tricornutum. Spectroscopic analysis proved that the more tightly bound FCP functions as a light-harvesting complex, actively transferring light energy from its accessory pigments chlorophyll c and fucoxanthin to the PSI core. Using an antibody against all FCP polypeptides of Cyclotella cryptica it could be shown that the polypeptides of the major FCP fraction differ from the FCPs found in the PSI fraction. Since these FCPs are tightly bound to PSI, active in energy transfer, and not found in the main FCP fraction, we suppose them to be PSI specific. Blue Native-PAGE, gel filtration and first electron microscopy studies of the PSI–FCP sample revealed a monomeric complex comparable in size and shape to the PSI–LHCI complex of green algae.

Plants were grown in field conditions in the wide area under normal water supply and severe water deficit. Two wheat (Triticum aestivum L.) genotypes contrasting by architectonics and differing in drought-resistance were used: Giymatli-2/17, short stature, with broad and drooping leaves, drought-sensitive, and Azamatli-95, short stature, with vertically oriented small leaves, drought-tolerant). It was found out that Giymatli-2/17 was characterized by relatively low content of Chl a-protein of PS I (CP I) and beta-subunit of ATP-synthase complex, the high content of proteins in the 33-30.5 kDa region and LHC polypeptides (28-24.5 kDa), the intensive fluorescence at 740 nm and more high photochemical activity of PS II under normal irrigation compared with Azamatli-95. However, the content of CP I (M(r) 115 kDa) and apoprotein of P700 with M(r) 63 kDa insignificantly increases in the drought-resistant genotype Azamatli-95 under extreme water supply condition while their content decreases in drought-sensitive cv Giymatli-2/17. Intensity of synthesis alpha- and beta-subunits of CF(1) (55 and 53.5 kDa) also decreases in Giymatli-2/17. The levels of the core antenna polypeptides of FS II with M(r) 46 and 44.5 kDa (CP47 and CP43) remains stable both in normal, and stressful conditions. At the same time the significant reduction is observed in the content of polypeptides in the 33-30.5 kDa region in the more sensitive genotype Giymatli-2/17. There is an increase in the LHC II polypeptides level in tolerant genotype Azamatli-95 in contrast to Giymatli-2/17 (where the content of these subunits is observed decreasing). The intensity of short wavelength peaks at 687 and 695 nm sharply increases in the fluorescence spectra (77 K) of chloroplasts from sensitive genotype Giymatli-2/17 under water deficiency and there is a stimulation of the ratio of fluorescence band intensity F687/F740. After exposure to drought, cv Giymatli-2/17 shows a larger reduction in the actual PS II photochemical efficiency of chloroplasts than cv Azamatli-95.

The definitive version is available at: http://www.sciencedirect.com/science//journal/00052728, Anomalies in photosynthetic activity of the soybean cell line STR7, carrying a single mutation (S268P) in the chloroplastic gene psbA that codes for the D1 protein of the photosystem II, have been examined using different spectroscopic techniques. Thermoluminescence emission experiments have shown important differences between STR7 mutant and wild type cells. The afterglow band induced by both white light flashes and far-red continuous illumination was downshifted by about 4 °C and the Q band was upshifted by 5 °C. High temperature thermoluminescence measurements suggested a higher level of lipid peroxidation in mutant thylakoid membranes. In addition, the reduction rate of P700+ was significantly accelerated in STR7 suggesting that the mutation led to an activation of the photosystem I cyclic electron flow. Modulated fluorescence measurements performed at room temperature as well as fluorescence emission spectra at 77 K revealed that the STR7 mutant is defective in state transitions. Here, we discuss the hypothesis that activation of the cyclic electron flow in STR7 cells may be a mechanism to compensate the reduced activity of photosystem II caused by the mutation. We also propose that the impaired state transitions in the STR7 cells may be due to alterations in thylakoid membrane properties induced by a low content of unsaturated lipids., This work was supported by grants from the Ministry of Education and Culture of Spain (BFU-BMC2004-04914-C02-01, BMC2002-00031 and BFU-BMC2005-07422-C02-01) and Andalusia Government (PAI CVI-261).

In this work, we investigated electron transport processes in the cyanobacterium Synechocystis sp. PCC 6803, with a special emphasis focused on oxygen-dependent interrelations between photosynthetic and respiratory electron transport chains. Redox transients of the photosystem I primary donor P700 and oxygen exchange processes were measured by the EPR method under the same experimental conditions. To discriminate between the factors controlling electron flow through photosynthetic and respiratory electron transport chains, we compared the P700 redox transients and oxygen exchange processes in wild type cells and mutants with impaired photosystem II and terminal oxidases (CtaI, CydAB, CtaDEII). It was shown that the rates of electron flow through both photosynthetic and respiratory electron transport chains strongly depended on the transmembrane proton gradient and oxygen concentration in cell suspension. Electron transport through photosystem I was controlled by two main mechanisms: (i) oxygen-dependent acceleration of electron transfer from photosystem I to NADP+, and (ii) slowing down of electron flow between photosystem II and photosystem I governed by the intrathylakoid pH. Inhibitor analysis of P700 redox transients led us to the conclusion that electron fluxes from dehydrogenases and from cyclic electron transport pathway comprise 20–30% of the total electron flux from the intersystem electron transport chain to P700+.

Electron paramagnetic resonance (EPR) was used to quantify Photosystem I (PSI) and PSII in vesicles originating from a series of well-defined but different domains of the thylakoid membrane in spinach prepared by non-detergent techniques. Thylakoids from spinach were fragmented by sonication and separated by aqueous polymer two-phase partitioning into vesicles originating from grana and stroma lamellae. The grana vesicles were further sonicated and separated into two vesicle preparations originating from the grana margins and the appressed domains of grana (the grana core), respectively. PSI and PSII were determined in the same samples from the maximal size of the EPR signal from P700(+) and Y-D(.), respectively. The following PSI/PSII ratios were found: thylakoids, 1.13; grana vesicles, 0.43; grana core, 0.25; grana margins, 1.28; stroma lamellae 3.10. In a sub-fraction of the stroma lamellae, denoted Y-100, PSI was highly enriched and the PSI/PSII ratio was 13. The antenna size of the respective photosystems was calculated from the experimental data and the assumption that a PSII center in the stroma lamellae (PSIIbeta) has an antenna size of 100 Ch1. This gave the following results: PSI in grana margins (PSIalpha) 300, PSI (PSIbeta) in stroma lamellae 214, PSII in grana core (PSIIalpha) 280. The results suggest that PSI in grana margins have two additional light-harvesting complex 11 (LHCII) trimers per reaction center compared to PSI in stroma lamellae, and that PSII in grana has four LHCII trimers per monomer compared to PSII in stroma lamellae. Calculation of the total chlorophyll associated with PSI and PSII, respectively, suggests that more chlorophyll (about 10%) is associated with PSI than with PSII. (C) 2003 Elsevier B.V. All rights reserved. (Less)

The cyanobacterium Synechococcus PCC 7942 grown under iron starvation assembles a supercomplex consisting of a trimeric Photosystem I (PSI) complex encircled by a ring of 18 CP43′ or IsiA complexes. It has previously been shown that PSI of Synechococcus PCC 7942 contains less special long-wavelength ('red') chlorophylls than PSI of most other cyanobacteria. Here we present a comparative analysis by time-resolved absorption difference and fluorescence spectroscopy of the processes of energy transfer and trapping in trimeric PSI and PSI-IsiA supercomplexes from Synechococcus PCC 7942. All experiments were performed with the primary electron donor of PSI (P700) in the oxidized state. Our data suggest that in the PSI complex the excitation energy is equilibrated with a lifetime of 0.6 ps among the so-called bulk chlorophylls, is distributed in 3-4 ps between the bulk and red chlorophylls, and is trapped in the reaction center in 19 ps. This trapping time is shorter than that observed for other cyanobacteria, which we attribute to the lower content of red chlorophylls in PSI of this organism. In the PSI-IsiA supercomplexes, the distribution of excited states is blue-shifted compared to that in PSI, leading to a lengthening of the equilibration processes. We attributed a phase of about 1 ps to initial energy equilibration steps among the IsiA and PSI core bulk chlorophylls, a 5-7 ps phase to equilibration between bulk and red chlorophylls within the PSI core, and a 38 ps phase to trapping in the reaction center. The data suggest that the excitation energy is equilibrated among the IsiA and PSI core antenna chlorophylls before trapping occurs. Data analysis based on a simple kinetic model revealed an intrinsic rate constant for energy transfer from IsiA to PSI in the range of 2±1 ps. Based on this value we suggest the presence of one or more linker chlorophylls between the IsiA and PSI core complexes. These results confirm that IsiA acts as an effective light-harvesting antenna for PSI. © 2004 Elsevier B.V. All rights reserved.

The roles of Ca(2+) in H(2)O oxidation may be as a site of substrate binding, and as a structural component of the photosystem II O(2)-evolving complex. One indication of this dual role of the metal is revealed by probing the Mn cluster in the Ca(2+) depleted O(2) evolving complex that retains extrinsic 23- and 17-kDa polypeptides with reductants (NH(2)OH and hydroquinone) [Biochemistry 41 (2002) 958]. Calcium appears to bind to photosystem II at a site where it could bind substrate H(2)O. Equilibration of Ca(2+) with this binding site is facilitated by increased ionic strength, and incubation of Ca(2+) reconstitution mixtures at 22 degrees C accelerates equilibration of Ca(2+) with the site. The Ca(2+) reconstituted enzyme system regains properties of unperturbed photosystem II: Sensitivity to NH(2)OH inhibition is decreased, and Cl(-) binding with increased affinity can be detected. The ability of ionic strength and temperature to facilitate rebinding of Ca(2+) to the intact O(2) evolving complex suggests that the structural environment of the oxidizing side of photosystem II may be flexible, rather than rigid.

The temperature dependence of the biphasic electron transfer (ET) from the secondary acceptor A1 (phylloquinone) to iron–sulfur cluster F X was investigated by flash absorption spectroscopy in photosystem I (PS I) isolated from Synechocystis sp. PCC 6803. While the slower phase ( τ =340 ns at 295 K) slowed upon cooling according to an activation energy of 110 meV, the time constant of the faster phase ( τ =11 ns at 295 K) was virtually independent of temperature. Following a suggestion in the literature that the two phases arise from bidirectional ET involving two symmetrically arranged phylloquinones, Q K -A and Q K -B, it is concluded that energetic parameters (most likely the driving forces) rather than the electronic couplings are different for ET from Q K -A to F X and from Q K -B to F X . Two alternative schemes of ET in PS I are presented and discussed.

Photoaccumulation of membrane preparations of Chlamydomonas reinhardtii at pH 8 and 220 K reduces the primary and secondary electron acceptors in the Photosystem I (PSI) reaction centre, and produces a maximum of two spins per P700 + . Proton electron nuclear double resonance (ENDOR) spectra demonstrate that the phyllosemiquinone produced is that attributed to the PsaA branch of electron transfer. Photoaccumulation at pH 10 and 220 K produces a maximum of four spins per P700 + , and proton ENDOR spectra indicate that a second phyllosemiquinone is being photoaccumulated, with markedly different proton hyperfine couplings (hfcs). This phyllosemiquinone is unaffected by mutation of PsaAW693, confirming that it does not arise from the PsaA branch of electron transfer, and we therefore attribute it to the PsaB phyllosemiquinone.

This mini-review focuses on recent experimental results and questions, which came up since the last more comprehensive reviews on the subject. We include a brief discussion of the different techniques used for time-resolved studies of electron transfer in photosystem I (PS I) and relate the kinetic results to new structural data of the PS I reaction centre.

The photosystem (PS) I photosynthetic reaction center was modified thorough the selective extraction and exchange of chlorophylls and quinones. Extraction of lyophilized photosystem I complex with diethyl ether depleted more than 90% chlorophyll (Chl) molecules bound to the complex, preserving the photochemical electron transfer activity from the primary electron donor P700 to the acceptor chlorophyll A(0). The treatment extracted all the carotenoids and the secondary acceptor phylloquinone (A(1)), and produced a PS I reaction center that contains nine molecules of Chls including P700 and A(0), and three Fe-S clusters (F(X), F(A) and F(B)). The ether-extracted PS I complex showed fast electron transfer from P700 to A(0) as it is, and to FeS clusters if phylloquinone or an appropriate artificial quinone was reconstituted as A(1). The ether-extracted PS I enabled accurate detection of the primary photoreactions with little disturbance from the absorbance changes of the bulk pigments. The quinone reconstitution created the new reactions between the artificial cofactors and the intrinsic components with altered energy gaps. We review the studies done in the ether-extracted PS I complex including chlorophyll forms of the core moiety of PS I, fluorescence of P700, reaction rate between A(0) and reconstituted A(1), and the fast electron transfer from P700 to A(0). Natural exchange of chlorophyll a to 710-740 nm absorbing chlorophyll d in PS I of the newly found cyanobacteria-like organism Acaryochloris marina was also reviewed. Based on the results of exchange studies in different systems, designs of photosynthetic reaction centers are discussed.

Thylakoids isolated from tobacco were fragmented by sonication and the vesicles so obtained were separated by partitioning in aqueous polymer two-phase systems. By this procedure, grana vesicles were separated from stroma exposed membrane vesicles. The latter vesicles could be further fractionated by countercurrent distribution, with dextran–polyethylene glycol phase systems, and divided into two main populations, tentatively named ‘stroma lamellae’ and ‘end membrane’. Both these vesicle preparations have high chlorophyll a/b ratio, high photosystem (PS) I and low PS II content, suggesting their origin from stroma exposed regions of the thylakoid. The two vesicle populations have been compared with respect to biochemical composition and photosynthetic activity. The ‘end membrane’ has a higher chlorophyll a/b ratio (5.7 vs. 4.7), higher P700 content (4.7 vs. 3.3 mmol/mol of chlorophyll). The ‘end membrane’ has the lowest PS II content, the ratio PS I/PS II being more than 10, as shown by EPR measurements. The PS II in both fractions is of the β-type. The decay of fluorescence is different for the two populations, the ‘stroma lamellae’ showing a very slow decay even in the presence of K3Fe(CN)6 as an acceptor. The two vesicle populations have very different surface properties: the end membranes prefer the upper phase much more than the stroma lamellae, a fact which was utilized for their separation. Arguments are presented which support the suggestion that the two vesicle populations originate from the grana end membranes and the stroma lamellae, respectively.

Six different spinach plastocyanin mutants have been constructed by site-directed mutagenesis and expressed in Escherichia coli to probe the importance of the two acidic patches in the interaction with photosystem I. The mutants were: Asp42Lys, Glu43Asn, Glu43Lys, Glu43Gln/Asp44Asn, Glu59Lys/Glu60Gln and Glu43Asn/Glu59Lys/Glu60Gln and they have been characterised by optical absorption and EPR spectroscopy, redox titrations and isoelectric focusing. The electron transfer to photosystem I was investigated by flash-induced time-resolved absorption measurements at 830nm. The kinetics were interpreted with a model that incorporates a rate-limiting conformational change from inactive to active forms of the plastocyanin-photosystem I complex. All mutations resulted in a displacement of the equilibrium towards the inactive conformation. The strongest impairment of the electron transfer was found for mutations in the larger acidic patch, in particular upon modification of residues 43 or 44. However, mutations of residues 59 and 60 in the smaller acidic patch also resulted in a lower reactivity.

Measurements of relative quantum yields of Photosystem II and Photosystem I partial reactions and room-temperature chlorophyll a fluorescence of thylakoids in high- and low-salt media showed that the cation-induced changes in the excitation energy distribution were inhibited in the thylakoids isolated from pea plants grown in the presence of sublethal concentration of the pyridazinone herbicide BASF 13.338. Simultaneous measurement of Photosystem II and Photosystem I fluorescence emission kinetics at 77 K showed that the ability of cations to regulate excitation energy spillover from Photosystem II to Photosystem I was inhibited in thylakoids of the BASF-grown plants. Cation regulation of the absorption cross-section of the photosystems was not affected. Electron microscope data revealed that the proportion of stroma membranes relative to grana membranes was markedly less in the thylakoids of the BASF-grown plants. Furthermore, when the thylakoids were resuspended in low-salt medium, no unstacking of the grana was detected. The observed inhibition of cation-induced spillover change was presumably due to loss of ability of these photosynthetic membranes to undergo unstacking in low-salt medium. Correspondence: S. Bose, National Institutes of Health, 9000 Rockville Pike, Building 3, Room Bl-22, Bethesda, MD 20892, USA.

N-terminal amino acid sequencing was carried out to characterize the genes of the cucumber PS I complex (PSI-100) that contains eight polypeptides and catalyzes the light-dependent transfer of electrons from plastocyanin to ferredoxin. The genes of all subunits except the 17.5 kDa polypeptide in PSI-100 have been identified. These are psaA/psaB (65/63 kDa), psaD (20 kDa), psaE (19.5 kDa), psaF (18.5 kDa), psaH (7.6 kDa), and psaC (5.8 kDa). The 17.5 kDa polypeptide is a new protein and is designated tentatively as the gene product of psaM. N-terminal amino-acid sequencing indicated the presence of two polypeptides in the 7.6 kDa band. One of these is the gene product of psaH and is essential for the activity of the PS I complex, and the other one is as yet unrecognized and largely depleted in the PSI-100 complex. Gene products of psaG, psaI, and psaK, which have been proposed as the components of PS I complex, are not involved in the PSI-100 complex, but are involved in the PS I complex (PSI-200), which contains 120 chlorophyll per reaction center chlorophyll (P700) and light-harvesting chlorophyll a/b protein complexes. Three polypeptides (26,23 and 22.5 kDa) are not involved in the PSI-100 and are assigned as the apo-protein of light-harvesting chlorophyll a/b protein complexes.

Electron paramagnetic resonance (EPR) spectra were recorded of whole filaments of the cyanobacteria Nostoc muscorum and Anabaena cylindrica . Signals due to manganese were removed by freezing and thawing the cells in EDTA. EPR spectra were assigned on the basis of their g values, linewidths, temperature dependence and response to dithionite and light treatments. The principal components identified were: (i) rhombic Fe 3+ (signal at g = 4.3), probably a soluble storage form of iron; (ii) iron-sulfur centers A and B of Photosystem I; (iii) the photochemical electron acceptor ‘X’ of Photosystem I; this component was also observed for the first time in isolated heterocysts; (iv) soluble ferredoxin which was present at a concentration of 1 molecule per 140 ± 20 chlorophyll molecules; (v) a membrane-bound iron-sulfur protein ( g = 1.92). A signal g = 6 in the oxidized state was probably due to an unidentified heme compound. During deprivation of iron the rhombic Fe 3+ , centers A, B and X of Photosystem I, and soluble ferredoxin were all observed to decrease.

A comparative study is made, at 15 degrees C, of flash-induced absorption changes around 820 nm (attributed to the primary donors of Photosystems I and II) and 705 nm (Photosystem I only), in normal chloroplasts and in chloroplasts where O2 evolution was inhibited by low pH or by Tris-treatment. At pH 7.5, with untreated chloroplasts, the absorption changes around 820 nm are shown to be due to P-700 alone. Any contribution of the primary donor of Photosystem II should be in times shorter than 60 mus. When chloroplasts are inhibited at the donor side of Photosystem II by low pH, an additional absorption change at 820 nm appears with an amplitude which, at pH 4.0, is slightly higher than the signal due to oxidized P-700. This additional signal is attributed to the primary donor of Photosystem II. It decays (t 1/2 about 180 mus) mainly by back reaction with the primary acceptor and partly by reduction by another electron donor. Acid-washed chloroplasts resuspended at pH 7.5 still present the signal due to Photosystem II (t 1/2 about 120 mus). This shows that the acid inhibition of the first secondary donor of Photosystem II is irreversible. In Tris-treated chloroplasts, absorption changes at 820 nm due to the primary donor of Photosystem II are also observed, but to a lesser extent and only after some charge accumulation at the donor side. They decay with a half-time of 120 mus.

Picosecond time-resolved fluorescence spectroscopy has been used to investigate the fluorescence emission from wild-type barley chloroplasts and from chloroplasts of the barley mutant, chlorina f-2, which lacks the light-harvesting chlorophyll a/b -protein complex. Cation-controlled regulation of the distribution of excitation energy was studied in isolated chloroplasts at the F 0 and F m levels. It was found that: 1. (a) The fluorescence decay curves were distinctly non-exponential, even at low excitation intensities ( 14 photons · cm −2 ). 2. (b) The fluorescence decay curves could, however, be described by a dual exponential decay law. The wild-type barley chloroplasts gave a short-lived fluorescence component of approximately 140 ps and a long-lived component of 600 ps ( F 0 ) or 1300 ps ( F m ) in the presence of Mg 2+ ; in comparison, the mutant barley yielded a short-lived fluorescence component of approx. 50 ps and a long-lived component of 194 ps ( F 0 ) and 424 ps ( F m ). 3. (c) The absence of the light-harvesting chlorophyll a/b -protein complex in the mutant results in a low fluorescence quantum yield which is unaffected by the cation composition of the medium. 4. (d) The fluorescence yield changes seen in steady-state experiments on closing Photosystem II reaction centres ( F m / F 0 ) or on the addition of MgCl 2 (+Mg 2+ /−Mg 2+ ) were in overall agreement with those calculated from the time-resolved fluorescence measurements. The results suggest that the short-lived fluorescence component is partly attributable to the chlorophyll a antenna of Photosystem I, and, in part, to those light-harvesting-Photosystem II pigment combinations which are strongly coupled to the Photosystem I antenna chlorophyll. The long-lived fluorescence component can be ascribed to the light-harvesting-Photosystem II pigment combinations not coupled with the antenna of Photosystem I. In the case of the mutant, the two components appear to be the separate emissions from the Photosystem I and Photosystem II antenna chlorophylls.

The extent of P -700 photooxidation at 18 °K has been followed in three different chloroplast preparations (unfractionated chloroplasts and two preparations enriched in Photosystem I). More than 90% of P -700 + formation in all preparations was eliminated by the addition of sodium dithionite at pH 10. Photoreduction of a bound chloroplast iron-sulfur protein was also decreased by at least 90% under similar conditions. Electron paramagnetic resonance spectra of the chloroplast preparations in the presence of dithionite showed chemical reduction of bound iron-sulfur protein under conditions where primary photochemistry is eliminated. These results indicate that P -700 photooxidation is concomitant with photoreduction of a bound iron-sulfur protein and that this iron-sulfur protein functions as the primary electron acceptor of Photosystem I.

The fluorescent emission kinetics of spinach subchloroplast Photosystems I and II particles have been studied on a picosecond time scale. Using picosecond laser pulses and an optical Kerr gate, the fluorescent decay times are measured to be 60 plus or minus 10 ps, and 200 plus or minus 20 ps for Photosystems I and II, respectively. The quantum yields are calculated to be 0.004 for Photosystem I and 0.013 for Photosystem II. Theory of exciton energy transfer and trapping is applied for the determination of intermolecular potential energyin the photosystems.

Flash-induced absorption changes of Triton-solubilized Photosystem I particles from spinach were studied under reducing and/or illumination conditions that serve to alter the state of bound electron acceptors. By monitoring the decay of P -700 following each of a train of flashes, we found that P -430 or components resembling it can hold 2 equivalents of electrons transferred upon successive illuminations. This requires the presence of a good electron donor, reduced phenazine methosulfate or neutral red, otherwise the back reaction of P -700 + with P -430 occurs in about 30 ms. If the two P -430 sites, designated Centers A and B, are first reduced by preilluminating flashes or chemically by dithionite under anaerobic conditions, then subsequent laser flashes generate a 250 μs back reaction of P -700 + , which we associate with a more primary electron acceptor A 2 . In turn, when A 2 is reduced by background (continuous) illumination in presence of neutral red and under strongly reducing conditions, laser flashes then produce a much faster (3 μs) back reaction at wavelengths characteristic of P -700. We associate this with another more primary electron acceptor, A 1 , which functions very close to P -700. The organization of these components probably corresponds to the sequence P-700- A 1 - A 2 -P-430[ A B ] . The relation of the optical components to acceptor species detected by EPR, by electron-spin polarization or in terms of peptide components of Photosystem I is discussed. Preliminary experiments with broken chloroplasts suggest that an analogous situation occurs there, as well.

The potassium salt-induced transient increase of delayed fluorescence yield was studied in pea chloroplasts treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea. A simple kinetic model is proposed to account for the actinic light intensity dependence of the delayed fluorescence enhancement by the transmembrane diffusion potential induced by sudden salt addition. The electric field dependence of the rate constants for the recombination of primary separated charges with and without subsequent electronic excitation of reaction center chlorophyll was obtained. From the value of enhancement of delayed fluorescence by salt concentration gradients at saturating actinic light intensity, it is concluded that the distance, normal to thylakoid membrane surface, between the primary acceptor and the donor of Photosystem II is smaller than the membrane thickness.

Light-induced absorption changes associated with the primary photochemical reaction and dark relaxation in Photosystem I were measured at various low temperatures. A possible temperature-dependent long-range electron tunneling process was suggested to account for the unique temperature dependence of the dark decay process. The kinetics of the light-induced absorption changes are in good agreement with the light-induced EPR changes reported earlier (Ke, B., Sugahara, K., Shaw, E.R., Hansen, R. E., Hamilton, W. D. and Beinert, H. (1974) Biochim. Biophys. Acta 368, 401–408) for the same Photosystem I subchloroplast fragments at comparable temperatures. All absorption changes between 400 and 725 nm at 86 °K have identical kinetics. The light-minus-dark difference spectrum is very similar to that of P -700 at room temperature, with an additional prominent positive change at 690 nm. Possible contributions by P -430 to the blue and red spectral changes were discussed. It was demonstrated that the intensity of the measuring beam has a drastic effect on the light-induced absorption changes of Photosystem I at low temperatures. Various pretreatments of the Photosystem I fragments such as those that photochemically (or chemically) oxidize the primary donor or photoreduce the primary acceptor abolish the subsequent photochemical reaction. Continuous illumination of the Photosystem I fragments before and during freezing has the same effect. In the temperature range of −20 to −60 °C, an unusual counter absorption change as well as a counter EPR change were observed.

1. By using dibromothymoquinone as the electron acceptor, it is possible to isolate functionally that segment of the chloroplast electron transport chain which includes only Photosystem II and only one of the two energy conservation sites coupled to the complete chain (Coupling Site II, observed P e 2 = 0.3–0.4 ). A light-dependent, reversible proton translocation reaction is associated with the electron transport pathway: H2O → Photosystem II → dibromothymoquinone. We have studied the characteristics of this proton uptake reaction and its relationship to the electron transport and ATP formation associated with Coupling Site II. 2. The initial phase of H+ uptake, analyzed by a flash-yield technique, exhibits linear kinetics (0–3 s) with no sign of transient phenomena such as the very rapid initial uptake (“pH gush”) encountered in the overall Hill reaction with methylviologen. Thus the initial rate of H+ uptake obtained by the flash-yield method is in good agreement with the initial rate estimated from a pH change tracing obtained under continuous illumination. 3. Dibromothymoquinone reduction, observed as O2 evolution by a similar flash-yield technique, is also linear for at least the first 5 s, the rate of O2 evolution agreeing well with the steady-state rate observed under continuous illumination. 4. Such measurements of the initial rates of O2 evolution and H+ uptake yield an H + e − ratio close to 0.5 for the Photosystem II partial reaction regardless of pH from 6 to 8. (Parallel experiments for the methylviologen Hill reaction yield an H + e − ratio of 1.7 at pH 7.6.) 5. When dibromothymoquinone is being reduced, concurrent phosphorylation (or arsenylation) markedly lowers the extent of H+ uptake (by 40–60%). These data, unlike earlier data obtained using the overall Hill reaction, lend themselves to an unequivocal interpretation since phosphorylation does not alter the rate of electron transport in the Photosystem II partial reaction. ADP, Pi and hexokinase, when added individually, have no effect on proton uptake in this system. 6. The involvement of a proton uptake reaction with an H + e − ratio of 0.5 in the Photosystem II partial reaction H2O → Photosystem II → dibromothymoquinone strongly suggests that at least 50% of the protons produced by the oxidation of water are released to the inside of the thylakoid, thereby leading to an internal acidification. It is pointed out that the observed efficiencies for ATP formation (P/e2) and proton uptake ( H + e − ) associated with Coupling Site II can be most easily explained by the chemiosmotic hypothesis of energy coupling.

Fluorescence emission spectra of chloroplasts, initially frozen to--196 degrees C, were measured at various temperatures as the sample was allowed to warm. The 735 nm emission band attributed to fluorescence from Photosystem I was approx. 10-fold greater at--196 degrees C than at--78 degrees C. The initial rate of photooxidation of P-700 was also measured at--196 degrees C and--78 degrees C and was found to be approximately twice as large at the higher temperature. It is proposed that the 735 nm emission band is fluorescence from a long wavelength form of chlorophyll, C-705, which acts as a trap for excitation energy in the antenna chlorophyl system of Photosystem I. Furthermore, it is proposed that C-705 only forms on cooling to low temperatures and that the temperature dependence of the 735 nm emission is the temperature dependence for the formation of C-705. C-705 and P-700 compete to trap the excitation energy in Photosystem I. It is estimated from the data that at--78 degrees C P-700 traps approx. 20 times more energy than C-705 while, at--196 degrees C, the two traps are approximately equally effective. By analogy, the 695 nm fluorescence which also appears on cooling to--196 degrees C is attributed to traps in Photosystem II which form only on cooling to temperatures near--196 degrees C.

The distribution of excitation energy in the photochemical apparatus of photosynthesis was examined with dark-grown bean leaves which had been partially greened by a series of brief xenon flashes. The yield of energy transfer from Photosystem II to Photosystem I was estimated by a method devised recently for spinach chloroplasts. Using that method, which involves a comparison of fluorescence excitation spectra with the absorption spectrum of the flashed leaves at −196 °C, the yield of energy transfer in the flashed leaves was found to be about twice the yield values obtained with chloroplasts. On further greening in continuous light, during which time the light-harvesting chlorophyll a / b protein accumulates, the yield of energy transfer decreases approaching the lower values found previously for spinach chloroplasts. The initial distribution of absorbed quanta between Photosystems I and II was also determined for the flashed leaves as a function of the wavelength of excitation. In contrast to spinach chloroplasts or to mature green leaves where that distribution is almost constant independent of wavelength at wavelengths shorter than 675 nm, the distribution of energy in the flashed leaves showed considerable variation with wavelength. The rate of photooxidation of P -700 at −196 °C was measured at two wavelengths, 645 and 670 nm, at which the initial distribution of energy between the photosystems is appreciably different. A comparison of the rates of photooxidation of P -700 with the relative intensities of Photosystem I fluorescence excited by these two wavelengths confirmed that energy was transferred from Photosystem II to Photosystem I and that the transferred energy stimulated both the photooxidation of P -700 and Photosystem I fluorescence at −196 °C.

The effects of lowering the pH on Photosystem II has been studied by measuring changes in absorbance and electron spin resonance in spinach chloroplasts. At pH values around 4 a light-induced dark-reversible chlorophyll oxidation by Photosystem II was observed. This chlorophyll is presumably the primary electron donor of system II. At pH values between 5 and 4 steady state illumination induced an ESR signal, similar in shape and amplitude to signal II, which was rapidly reversed in the dark. This may reflect the accumulation of the oxidized secondary donor upon inhibition of oxygen evolution. Near pH 4 the rapidly reversible signal and the stable and slowly decaying components of signal II disappeared irreversibly concomitant with the release of bound manganese. The results are discussed in relation to the effects of low pH on prompt and delayed fluorescence reported earlier (van Gorkom, H.J., Pulles, M.P.J., Haveman, J. and den Haan, G.A. (1976) Biochim. Biophys, Acta 423, 217-226).

Rates of photooxidation of P -700 by green (560 nm) or blue (438 nm) light were measured in whole cells of Porphyridium cruentum which had been frozen to −196 °C under conditions in which the Photosystem II reaction centers were either all open (dark adapted cells) or all closed (preilluminated cells). The rate of photooxidation of P -700 at −196 °C by green actinic light was approx. 80% faster in the preilluminated cells than in the dark-adapted cells. With blue actinic light, the rates of P -700 photooxidation in the dark-adapted and preilluminated cells were not significantly different. These results are in excellent agreement with predictions based on our previous estimates of energy distribution in the photosynthetic apparatus of Porphyridium cruentum including the yield of energy transfer from Photosystem II to Photosystem I determined from low temperature fluorescence measurements.

The MgCl2-induced chlorophyll fluorescence yield changes in broken chloroplasts, suspended in a cation-free medium, treated with 3,-(3',4'-dichlorophenyl)-1,1-dimethylurea and pre-illuminated, has been investigated on a pico-second time scale. Chloroplasts in the low fluorescing state showed a fluorescence decay law of the form exp --At1/2, where A was found to be 0.052 ps-1/2, and may be attributed to the rate of spillover from Photosystem II to Photosystem I. Addition of 10 mM MgCl2 produced a 50% increase in the steady-state fluorescence quantum yield and caused a marked decrease in the decay rate. The fluorescence deday law was found to be predominantly exponential with a 1/e lifetime of 1.6 ns. These results support the hypothesis that cation-induced changes in the fluorescence yield of chlorophyll are related to the variations in the rate of energy transfer from Photosystem II to Photosystem I, rather than to changes in the partitioning of absorbed quanta between the two systems.

Fractions enriched in either Photosystem I or Photosystem II have been prepared from chloroplasts with digitonin. A more detailed analysis of the decay kinetics of fluorescence excited by a picosecond laser pulse has been possible compared to experiments with unfractionated systems. The Photosystem I fractions show a very short component (less than or equal to 100 ps) at room temperature which is apparently independent of pulse intensity over the range of photon densities used (5 - 10(13)--1 - 10(16) photons cm-2). The Photosystem II fraction has a short initial lifetime at room temperature which is strongly intensity-dependent approaching 500 ps at low photon densities, but decreasing to close to 150 ps at the highest photon densities. All of these room temperature decays appear to be non-exponential, and may possibly be fitted by at t1/2 expression, expected from a random diffusion of excitations via Förster energy transfer. On cooling to 77K, lifetimes of both Photosystem I and Photosytem II increase, the lengthening with Photosystem I being more striking. The Photosystem I decays become intensity dependent like the Photosystem II, and at the lowest photon densities decays which are more nearly exponential within the experimental error give initial lifetimes of about 2 ns. The non-exponential decays seen at high photon densities appear to fit a t1/2 expression.

The following arguments in favor of exciton transfer between the two photosystems are presented: 1. (1) MgCl2 (1–10 mM range) decreases the intersystem transfer but does not modify the partition of absorbed photons between the photosystems. MgCl2 addition causes a simultaneous increase of excitation life time (τ) and of fluorescence intensity (F). The same linear relationship is obtained with or without added Mg2+. 2. (2) The deactivation of Photosystem II by the Photosystem II to Photosystem I transfer increases with the level of reduced Photosystem II traps. When all Photosystem II traps are closed, half of Photosystem II excitons are deactivated by transfer to Photosystem I. 3. (3) From the relative values of the 685-nm fluorescence yield and System II electron transport rate in limiting light, measured with and without MgCl2, the values of rate constants of Photosystem II deactivation were calculated. 4. (4) The intersystem transfer determines a 715-nm variable fluorescence, which is lowered by MgCl2 addition. When this transfer is decreased by MgCl2 the efficiency of the transfer between Photosystem II-connected units is enhanced, and a more sigmoidal fluorescence rise is obtained. A double-layer model of the thylakoid membrane where each photosystem is restricted to one leaflet is proposed to explain the decrease of the intersystem transfer after adding cations. It is suggested that MgCl2 decreases the thickness of the Photosystem I polar region, increasing the distance between the pigments of the two photosystems.

When isolated chloroplasts from mature pea (Pisum sativum) leaves were treated with digitonin under "low salt" conditions, the membranes were extensively solubilized into small subunits (as evidenced by analysis with small pore ultrafilters). From this solubilized preparation, a photochemically inactive chlorophyll - protein complex (chlorophyll alpha/beta ratio, 1.3) was isolated. We suggest that the detergent-derived membrane fragment from mature membranes is a structural complex within the membrane which contains the light-harvesting chlorophyll alpha/beta protein and which acts as a light-harvesting antenna primarily for Photosystem II. Cations dramatically alter the structural interaction of the light-harvesting complex with the photochemically active system II complex. This interaction has been measured by determining the amount of protein-bound chlorophyll beta and Photosystem II activity which can be released into dispersed subunits by digitonin treatment of chloroplast lamellae. When cations are present to cause interaction between the Photosystem II complex and the light-harvesting pigment - protein, the combined complexes pellet as a "heavy" membranous fraction during differential centrifugation of detergent treated lamellae. In the absence of cations, the two complexes dissociate and can be isolated in a "light" submembrane preparation from which the light-harvesting complex can be purified by sucrose gradient centrifugation. Cation effects on excitation energy distribution between Photosystems I and II have been monitored by following Photosystem II fluorescence changes under chloroplast incubation conditions identical to those used for detergent treatment (with the exception of chlorophyll concentration differences and omission of detergents). The cation dependency of the pigment - protein complex and Photosystem II reaction center interactions measured by detergent fractionation, and regulation of excitation energy distribution as measured by fluorescence changes, were identical. We conclude that changes in substructural organization of intact membranes, involving cation induced changes in the interaction of intramembranous subunits, are the primary factors regulating the distribution of excitation energy between Photosystems II and I.

Using dark adapted isolated spinach chloroplasts and sequences of brief saturating flashes the correlation of the uptake and release of protons with electron transport from Photosystem II to Photosystem I were studied. The following observations and conclusions are reported: (1) Flash-induced proton uptake shows a weak, damped binary oscillation, with maxima occurring after the 2nd, 4th, etc. flashes. The damping factor is comparable to that observed in the O2 flash yield oscillation and therefore explained by misses in Photosystem II. (2) On the average and after a steady state is reached, each flash (i.e. each reduction of Q) induces the uptake of 2H+ from outside the chloroplasts. (3) Flash induced proton release inside the chloroplast membrane shows a strong damped binary oscillation with maximum release occurring also after the 2nd, 4th, etc. flashes. (4) This phenomenon is correlated with the earlier reported binary oscillations of electron transport [2] and shows that both electrons and protons are transported in pairs between the photosystems. (5) In two sequential flashes 4H+ from the outside of the thylakoid and 2e- from water are accumulated at a binding site B. Subsequently, the two electrons are transferred to non-protonated acceptors in Photosystem I (probably plastocyanin and cytochrome f) and the 4H+ are released inside the thylakoid. (6) It is concluded that a primary proton transporting site and/or energy conserving step located between the photosystems is being observed.

Light-induced changes of EPR signals in Photosystem-I subchloroplast particles at temperatures between 225 and 13 °K showed that the rates of onset of photooxidation of P700 and photoreduction of iron-sulfur protein(s) are identical and instantaneous within the limits of resolution of our instruments. The fraction of the P700+ EPR signal that appears reversibly decreased with decreasing temperature down to 13 °K when the photoreaction was completely irreversible. At temperatures below 225 °K, the reversible fraction consists of two approximately equal portions with decay halftimes of approx. 3 and 75 s, respectively. Light-induced absorption changes due to P700 photooxidation at low temperatures monitored at 700 nm showed a similar kinetic pattern. Since the reduced iron-sulfur protein signals can only be detected at very low temperature, their decay kinetics cannot be continuously monitored at higher temperatures. Therefore, exposure at appropriate temperatures and reaction times were selected according to the decay kinetics of P700+, after which decay was stopped by lowering the temperature to 13 °K and the P700+ and reduced iron-sulfur protein signals were recorded and compared. In the temperature range (225-13 °K) studied, the decay of P700+ and reduced iron-sulfur protein signals appears identical, suggesting that the two oppositely charged species recombine in the dark. These experiments support the view that iron-sulfur protein(s) is the reaction partner of P700 in the primary photochemical act of Photosystem I.

The kinetics of the fluorescence yield Ф of chlorophyll a in Chlorella pyrenoidosa were studied under anaerobic conditions in the time range from 50 μs to several minutes after short ( t 1 2 = 30 ns or 5 μs) saturating flashes. The fluorescence yield “in the dark” increased from Ф = 1 at the beginning to Ф ≈ 5 in about 3 h when single flashes separated by dark intervals of about 3 min were given. After one saturating flash, Ф increased to a maximum value (4–5) at 50 μs, then Ф decreased to about 3 with a half time of about 10 ms and to the initial value with a half time of about 2 s. When two flashes separated by 0.2 s were given, the first phase of the decrease after the second flash occurred within 2 ms. After one flash given at high initial fluorescence yield, the 10-ms decay was followed by a 10 s increase to the initial value. After the two flashes 0.2 s apart, the rapid decay was not follewed by a slow increase. These and other experiments provided additional evidence for and extend an earlier hypothesis concerning the acceptor complex of Photosystem II (Bouges-Bocquet, B. (1973) Biochim. Biophys. Acta 314, 250–256; Velthuys, B. R. and Amesz, J. (1974) Biochim. Biophys. Acta 333, 85–94): reaction center 2 contains an acceptor complex QR consisting of an electron-transferring primary acceptor molecule Q, and a secondary electron acceptor R, which can accept two electrons in succession, but transfers two electrons simultaneously to a molecule of the tertiary acceptor pool, containing plastoquinone (A). Furthermore, the kinetics indicate that 2 reactions centers of System I, excited by a short flash, cooperate directly or indirectly in oxidizing a plastohydroquinone molecule (A2−). If initially all components between photoreaction 1 and 2 are in the reduced state the following sequence of reactions occurs after a flash has oxidised A2− via System I: Q−R2− + A → Q−R + A2− → QR− + A2−. During anaerobiosis two slow reactions manifest themselves: the reduction of R (and A) within 1 s, presumably by an endogenous electron donor D1, and the reduction of Q in about 10 s when R is in the state R− and A in the state A2−. An endogenous electron donor, D2, and Q− compete in reducing the photooxidized donor complex of System II in reactions with half times of the order of 1 s.

The electron-transfer reactions between the plastoquinone molecules of the acceptor side of photosystem II have been inferred to be regulated by a proteinaceous component (apoenzyme), which additionally contains the receptor site for DCMU-type inhibitors (Renger, G., (1976) Biochim. Biophys. Acta 440, 287–300). In order to reveal the functional properties of this apoenzyme, the effect of procedures which modify the structure of proteins on the photosystem II electron transport have been investigated in isolated spinach chloroplasts by comparative measurements of O 2 evolution and absorption changes at 334 nm induced by repetitive flash excitation and of fluorescence induction curves caused by continuous actinic light. It was found that: (1) The release of blockage of O 2 evolution by the DCMU-type inhibitor SN 58132 due to mild tryptic digestion correlates kinetically with the deterioration of the binding properties. (2) Glutaraldehyde fixation of chloroplasts does not markedly modify the reoxidation kinetics of the reduced primary plastoquinone acceptor component, X320 − , of photosystem II, but it greatly reduces the fluorescence yield of the antenna chlorophylls and slightly retards the ADRY effect. Furthermore, it prevents the attack of trypsin on the apoenzyme. (3) Incubation of chloroplasts in ‘low’ salt medium markedly diminishes the ability of trypsin to release the blockage of O 2 evolution by SN 58132 and completely presents the effect on inhibition by DCMU. Based on these results and taking into account recent findings of other groups, the functional mechanism of the electron transport on the acceptor side of photosystem II is discussed. Assuming a tunnel mechanism, the apoprotein is inferred to act as a dynamic regulator rather than changing only the relative levels of the redox potentials of the plastoquinone molecules involved in the transfer steps. It is further concluded that salt depletion does not only cause grana unstacking and a change of the excitation energy transfer probabilities, but it additionally modifies the orientation of functional membrane proteins of photosystem II and their structural interaction within the thylakoid membrane.

Fluorescence emission spectra excited at 514 and 633 nm were measured at -196 degrees C on dark-grown bean leaves which had been partially greened by a repetitive series of brief xenon flashes. Excitation at 514 nm resulted in a greater relative enrichment of the 730 nm emission band of Photosystem I than was obtained with 633 nm excitation. The difference spectrum between the 514 nm excited fluorescence and the 633 nm excited fluorescence was taken to be representative of a pure Photosystem I emission spectrum at -196 degrees C. It was estimated from an extrapolation of low temperature emission spectra taken from a series of flashed leaves of different chlorophyll content that the emission from Photosystem II at 730 nm was 12% of the peak emission at 694 nm. Using this estimate, the pure Photosystem I emission spectrum was subtracted from the measured emission spectrum of a flashed leaf to give an emission spectrum representative of pure Photosystem II fluorescence at -196 degrees C. Emission spectra were also measured on flashed leaves which had been illuminated for several hours in continuous light. Appreciable amounts of the light-harvesting chlorophyll a/b protein, which has a low temperature fluorescence emission maximum at 682 nm, accumulate during greening in continuous light. The emission spectra of Photosystem I and Photosystem II were subtracted from the measured emission spectrum of such a leaf to obtain the emission spectrum of the light-harvesting chlorophyll a/b protein at -196 degrees C.

The previously reported effect of salt concentration on the fluorescence and other photochemical activities of Photosystem II is interpreted in terms of a change in the radiationless transition and the trapping probabilities. This is confirmed by quantitative comparison of the fluorescence and the photochemical activity. As a by-product of this analysis a method is devised to estimate the background fluorescence. We did not eliminate the possibility that the radiationless transition constant may include a contribution of energy transfer from Photosystem II to Photosystem I.