Evidence for the role of the light-harvesting chlorophyll a/b protein complex in photosystem II heterogeneity

Analyses of chlorophyll fluorescence induction kinetics from DCMU-poisoned thylakoids were used to examine the contribution of the light-harvesting chlorophyll a/b protein complex (LHCP) to Photosystem II (PS II) heterogeneity. Thylakoids excited with 450 nm radiation exhibited fluorescence induction kinetics characteristic of major contributions from both PS II and PS II_β centres. On excitation at 550 nm the major contribution was from PS II_β centres, that from PS II centres was only minimal. Mg²⁺ depletion had negligible effect on the induction kinetics of thylakoids excited with 550 nm radiation, however, as expected, with 450 nm excitation a loss of the PS II component was observed. Thylakoids from a chlorophyll-b-less barley mutant exhibited similar induction kinetics with 450 and 550 nm excitation, which were characteristic of PS II_β centres being the major contributors; the PS II contribution was minimal. The fluorescence induction kinetics of wheat thylakoids at two different developmental stages, which exhibited different amounts of thylakoid appression but similar chlorophyll a/b ratios and thus similar PS II:LHCP ratios, showed no appreciable differences in the relative contributions of PS II and PS II_β centres. Mg²⁺ depletion had similar effects on the two thylakoid preparations. These data lead to the conclusion that it is the PS II:LHCP ratio, and probably not thylakoid appression, that is the major determinant of the relative contributions of PS II and PS II_β to the fluorescence induction kinetics. PS II characteristics are produced by LHCP association with PS II, whereas PS II_β characteristic can be generated by either disconnecting LHCP from PS II or by preferentially exciting PS II relative to LHCP.     

Spinach-thylakoid phosphorylation: Studies on the kinetics of changes in photosystem antenna size, spill-over and phosphorylation of light-harvesting chlorophyll a/b protein

The kinetics of LHCP phosphorylation and associated changes in photosystem cross-section and energy ‘spill-over’ from PS II to PS I have been examined in isolated spinach chloroplasts. During an initial phosphorylation period of 3–6 min, in the presence of saturating concentrations of Mg²⁺, the increase in PS I and decrease in PS II cross-section are largely completed, as judged by both measurements of the steady-state redox state of Q and fluorescence yield changes. This corresponds to a period of rapid ³²P incorporation into the low-molecular weight LHCP polypeptide. Subsequent to this initial 3–6-min period there is substantial further phosphorylation of both LHCP polypeptides, which is not accompanied by significant changes in photosystem cross-section, even after the chloroplasts had been unstacked with extensive mixing of PS I and PS II by Mg-removal. It is suggested that there exists a specific ‘mobile’ population of LHCP molecules which is rapidly phosphorylated and which may be enriched in the low-molecular-weight polypeptide. In addition, measurements of the kinetics of the ‘spill-over’ changes upon either Mg²⁺ addition or removal indicate that the continued phosphorylation of LHCP is able to increase the ‘spill-over’ process under favourable ionic conditions.     

Antenna structure and excitation dynamics in photosystem I. II. Studies with mutants of Chlamydomonas reinhardtii lacking photosystem II.

Using time-resolved single photon counting, fluorescence decay in photosystem I (PS I) was analyzed in mutant strains of Chlamydomonas reinhardtii that lack photosystem II. Two strains are compared: one with a wild-type PS I core antenna (120 chlorophyll a/P700) and a second showing an apparent reduction in core antenna size (60 chlorophyll a/P700). These data were calculated from the lifetimes of core antenna excited states (75 and 45 ps, respectively) and from pigment stoichiometries. Fluorescence decay in wild type PS I is composed of two components: a fast 75-ps decay that represents the photochemically limited lifetime of excited states in the core antenna, and a minor (less than 10%) 300-800 ps component that has spectral characteristics of both peripheral and core antenna pigments. Temporal and spectral properties of the fast PS I decay indicate that (a) excitations are nearly equilibrated among the range of spectral forms present in the PS I core antenna, (b) an average excitation visits a representative distribution of core antenna spectral forms on all pigment-binding subunits regardless of the origin of the excitation, (c) reduction in core antenna size does not alter the range of antenna spectral forms present, and (d) transfer from peripheral antennae to the PS I core complex is rapid (less than 5 ps).     

Difference picosecond spectroscopy of pigment-protein complexes of photosystem I from higher plants

Using a difference picosecond spectrophotometer with a time resolution of 10 ps, we investigated excitation energy transfer and charge separation in pigment-protein complexes of Photosystem I from bean leaves (chlorophyll/P-700 = 60). Under 20 ps excitation at 650 or 667 nm, the difference absorption spectra in the spectral region 600–720 nm were measured. They are associated with transition of antenna chlorophylls into singlet excited states and P-700 photooxidation. It was shown that the excited states in the whole inhomogeneous antenna were generated within 10 ps and deactivated with three-component kinetics, the t_1/e values being 20–45, 100–300 and over 500 ps. Formation of P-700⁺ has a rise time of 15–30 ps. The fast component of the depletion of the antenna excited states is suggested to be due to transfer of excitation energy from antenna pigments to reaction centers and its trapping. The kinetics of the fast component is independent of excitation energy and a redox state of P-700.     

Evidence for the role of the light-harvesting chlorophyll protein complex in photosystem II heterogeneity

Analyses of chlorophyll fluorescence induction kinetics from DCMU-poisoned thylakoids were used to examine the contribution of the light-harvesting chlorophyll protein complex (LHCP) to Photosystem II (PS II) heterogeneity. Thylakoids excited with 450 nm radiation exhibited fluorescence induction kinetics characteristic of major contributions from both PS II_α and PS II_β centres. On excitation at 550 nm the major contribution was from PS II_β centres, that from PS II_α centres was only minimal. Mg²⁺ depletion had negligible effect on the induction kinetics of thylakoids excited with 550 nm radiation, however, as expected, with 450 nm excitation a loss of the PS II_α component was observed. Thylakoids from a chlorophyll-b-less barley mutant exhibited similar induction kinetics with 450 and 550 nm excitation, which were characteristic of PS II_β centres being the major contributors; the PS II_α contribution was minimal. The fluorescence induction kinetics of wheat thylakoids at two different developmental stages, which exhibited different amounts of thylakoid appression but similar chlorophyll ratios and thus similar PS II:LHCP ratios, showed no appreciable differences in the relative contributions of PS II_α and PS II_β centres. Mg²⁺ depletion had similar effects on the two thylakoid preparations. These data lead to the conclusion that it is the PS II:LHCP ratio, and probably not thylakoid appression, that is the major determinant of the relative contributions of PS II_α and PS II_β to the fluorescence induction kinetics. PS II_α characteristics are produced by LHCP association with PS II, whereas PS II_β characteristic can be generated by either disconnecting LHCP from PS II or by preferentially exciting PS II relative to LHCP.     

The significance of the kinetic analysis of fluorescence induction in DCMU-inhibited chloroplasts in terms of photosystem 2 connectivity and heterogeneity

A study has been made on the slow component (β_max) of chlorophyll fluorescence induction curves exhibited by DCMU-inhibited pea thylakoids. In the absence of high levels of screening cations, β_max is high and the fluorescence yield low, while the addition of K⁺, Mg²⁺ or Tris(ethylenediamine) cobaltic(III) cation (TEC³⁺) decreases β_max and increases fluorescence yield. These changes are inhibited when the thylakoids are fixed with glutaraldehyde. By comparing cation- and light-harvesting chlorophyll a/b-protein (LHCP) phosphorylation-induced changes it can be seen that β_max correlates with changes in the overall kinetics of photosystem (PS) 2 photoreduction, as indicated from the normalised area over the induction curve (Anorm). When the plastoquinone (PQ) pool is chemically reduced by dithionite, prior to the initiation of the curve, both F_o and F_m are increased and the slow component removed. These observations are used to question the concept of two structurally distinct PS2 centres [Arch. Biochem. Biophys. (1978) 190, 523–530] and to discuss the use of β_max in monitoring PS2 organisation.     

Excitation energy transfer in thylakoid membranes from Chlamydomonas reinhardtii lacking chlorophyll b and with mutant Photosystem I

Energy trapping in Photosystem I (PS I) was studied by time-resolved fluorescence spectroscopy of PS II-deleted Chl b-minus thylakoid membranes isolated from site-directed mutants of Chlamydomonas reinhardtii with specific amino acid substitutions of a histidine ligand to P₇₀₀. In vivo the fluorescence of the PS I core antenna in mutant thylakoids with His-656 of PsaB replaced by asparagine, serine or phenylalanine is characterized by an increase in the lifetime of the fast decay component ascribed to the energy trapping in PS I (25 ps in wild type PS I with intact histidine-656, 50 ps in the mutant PS I with asparagine-656 and 70 ps in the mutant PS I with phenylalanine-656). Assuming that the excitation dynamics in the PS I antenna are trap-limited, the increase in the trapping time suggests a decrease in the primary charge separation rate. Western blot analysis showed that the mutants accumulate significantly less PS I than wild type. Spectroscopically, the mutations lead to a decrease in relative quantum yield of the trapping in the PS I core and increase in relative quantum yield of the fluorescence decay phase ascribed to uncoupled chlorophyll–protein complexes which suggests that improper assembly of PS I and LHC in the mutant thylakoids may result in energy uncoupling in PS I.     

Chlorophyll fluorescence changes at high temperatures induced by linear heating of greening barley leaves

A relative decrease of the high temperature part (above 60°C) of the chlorophyll fluorescence temperature curve during 3 h to 10 h greening period of barley (Hordeum vulgare L.) leaves was found to be concomitant to a decrease of Chl alb ratio and to a gradual increase of LHCP/core ratio found by electrophoresis and the ratio of granal to total length of thylakoid membranes. It is suggested that the high temperature part of the fluorescence temperature curve depends inversely on the relative amount of LHC II in thylakoid membranes.Abbreviations Chl a(b) chlorophyll a(b) - CPa chlorophyll a protein complex of PS II - CP1 P700 chlorophyll a protein complex of PS I - FP free pigments - FTC fluorescence temperature curve - F(T30) fluorescence intensity at 30°C - LHC II light harvesting complex II - LHCP light harvesting chlorophyll protein - LHCP3 (LHCPm) monomeric form of LHC II - LHCPo oligomeric form of LHC II complex - M1 first maximum of FTC - M2 second maximum (region) of FTC - PAA polyacrylamide - PAR photosynthetically active radiation - PS I(II) Photosystem I(II) - SDS-PAGE sodium dodecyl sulfate polyacrylamide gel electrophoresis     

Energy equilibration and primary charge separation in chlorophyll d-based photosystem I reaction center isolated from Acaryochloris marina

Primary photochemistry in photosystem I (PS I) reaction center complex from Acaryochloris marina that uses chlorophyll d instead of chlorophyll a has been studied with a femtosecond spectroscopy. Upon excitation at 630 nm, almost full excitation equilibration among antenna chlorophylls and 40% of the excitation quenching by the reaction center are completed with time constants of 0.6(±0.1) and 4.9(±0.6) ps, respectively. The rise and decay of the primary charge-separated state proceed with apparent time constants of 7.2(±0.9) and 50(±10) ps, suggesting the reduction of the primary electron acceptor chlorophyll (A₀) and its reoxidation by phylloquinone (A₁), respectively.     

Light-induced quenching of chlorophyll fluorescence at 77 K in leaves,chloroplasts and Photosystem II particles

The light-induced chlorophyll (Chl) fluorescence decline at 77 K was investigated in segments of leaves, isolated thylakoids or Photosystem (PS) II particles. The intensity of chlorophyll fluorescence declines by about 40% upon 16 min of irradiation with 1000 μmol m⁻² s⁻¹ of white light. The decline follows biphasic kinetics, which can be fitted by two exponentials with amplitudes of approximately 20 and 22% and decay times of 0.42 and 4.6 min, respectively. The decline is stable at 77 K, however, it is reversed by warming of samples up to 270 K. This proves that the decline is caused by quenching of fluorescence and not by pigment photodegradation. The quantum yield for the induction of the fluorescence decline is by four to five orders lower than the quantum yield of Q_A reduction. Fluorescence quenching is only slightly affected by addition of ferricyanide or dithionite which are known to prevent or stimulate the light-induced accumulation of reduced pheophytin (Pheo). The normalised spectrum of the fluorescence quenching has two maxima at 685 and 695 nm for PS II emission and a plateau for PS I emission showing that the major quenching occurs within PS II. ‘Light-minus-dark’ difference absorbance spectra in the blue spectral region show an electrochromic shift for all samples. No absorbance change indicating Chl oxidation or Pheo reduction is observed in the blue (410–600 nm) and near infrared (730–900 nm) spectral regions. Absorbance change in the red spectral region shows a broad-band decrease at approximately 680 nm for thylakoids or two narrow bands at 677 and 670–672 nm for PS II particles, likely resulting also from electrochromism. These absorbance changes follow the slow component of the fluorescence decline. No absorbance changes corresponding to the fast component are found between 410 and 900 nm. This proves that the two components of the fluorescence decline reflect the formation of two different quenchers. The slow component of the light-induced fluorescence decline at 77 K is related to charge accumulation on a non-pigment molecule of the PS II complex. This revised version was published online in June 2006 with corrections to the Cover Date.     

The Regulation and Distribution of LHC-I and LHCP2 between the Photosystem I and Photosystem II

Evidences were provided in this paper that the relative distribution of chl-protein complexes of PSⅠ and PSⅡ could be regulated by Mg2+. addition of Mg2+ led to decrease in the amount of chl-protein complexes of PSⅠ and increase in the amount of chl-protein in complexes of PSⅡ. There was no effect of Mg2+ on the spectral property of LHCP1, but the addition of Mg2+ could change the spectral property of LHCP2 so that it became similar to that of the LHC-Ⅰ. CPIa2 was a complex of reaction centre of PSⅠ and LHC-I. LHC-I might be contacted specially with LHCP2 in chloroplast membranes. Addition of Mg2+ probably cansed the motion of LHC-I from PSⅠ to PSⅡ and became more closely connected with LHCP2. The relative amount of CPIa2, CPIa1, LHCP1 and LHCP2 in chloroplast membranes could be regulated by different light intensity. There were more CPIa2, LHCP1 and less LHCP2 in chloroplast membranes from the shade plant Malaxis monophyllos and sunflower grown under weak light, both of them lacked equally CPIa1. There were less CPIa2, LHCP1 and more LHCP2 in the sun plant spinach and sunflower grown under strong light, and they possessed equally CPIa1 chl-protein complexes. It is suggested that LHCP1 and LHCP2 are different light-harvesting Chl-protein complexes. The LHC-I and LHCP2 are mobile light-harvesting chl-protein complexes and shuttle back and forth between PSⅠ and PSⅡ They play an important role in the regulation and distribution of excitation energy between the two photosystems.     

Energy and electron transfer in photosystem II of a chlorophyll b-containing Synechocystis sp. PCC 6803 mutant

Using a Synechocystis sp. PCC 6803 mutant strain that lacks photosystem (PS) I and that synthesizes chlorophyll (Chl) b, a pigment that is not naturally present in the wild-type cyanobacterium, the functional consequences of incorporation of this pigment into the PS II core complex were investigated. Despite substitution of up to 75% of the Chl a in the PS II core complex by Chl b, the modified PS II centers remained essentially functional and were able to oxidize water and reduce Q(A), even upon selective excitation of Chl b at 460 nm. Time-resolved fluorescence decay measurements upon Chl excitation showed a significant reduction in the amplitude of the 60-70 ps component of fluorescence decay in open Chl b-containing PS II centers. This may indicate slower energy transfer from the PS II core antenna to the reaction center pigments or slower energy trapping. Chl b and pheophytin b were present in isolated PS II reaction centers. Pheophytin b can be reversibly photoreduced, as evidenced from the absorption bleaching at approximately 440 and 650 nm upon illumination in the presence of dithionite. Upon excitation at 685 nm, transient absorption measurements using PS II particles showed some bleaching at 650 nm together with a major decrease in absorption around 678 nm. The 650 nm bleaching that developed within approximately 10 ps after the flash and then remained virtually unchanged for up to 1 ns was attributed to formation of reduced pheophytin b and oxidized Chl b in some PS II reaction centers. Chl b-containing PS II had a lower rate of charge recombination of Q(A)(-) with the donor side and a significantly decreased yield of delayed luminescence in the presence of DCMU. Taken together, the data suggest that Chl b and pheophytin b participate in electron-transfer reactions in PS II reaction centers of Chl b-containing mutant of Synechocystis without significant impairment of PS II function.     

Isolation of an oxygen-evolving Photosystem II preparation containing only one tightly bound calcium atom from a chlorophyll b-deficient mutant of rice

Oxygen-evolving Photosystem II (PS II) particles were prepared from the thylakoid membranes of a chlorophyll b-less rice mutant, which totally lacks light-harvesting chlorophyll a/b proteins, after solubilization with β-octylglucoside. The preparation was essentially free of Photosystem I as judged from its low-temperature fluorescence spectrum and polypeptide composition. The PS II particles contained all the major subunit polypeptides of the PS II reaction center core complexes and the three extrinsic proteins related to oxygen evolution. The relative abundances of the 33, 21 and 15 kDa proteins were 100, 64 and 20%, respectively, of the corresponding proteins in the mutant thylakoids. The chlorophyll-to-Q_A ratio was 53 and there was only one bound Ca²⁺ per Q_A. Thus, one of the two bound Ca²⁺ present in the oxygen-evolving PS II membrane preparations from wild-type rice (Shen J.-R., Satoh, K. and Katoh, S. (1988) Biochim. Biophys. Acta 933, 358–364) is missing. The mutant PS II particles were highly active in oxygen evolution in the absence of exogenously added Ca²⁺, although addition of 5 mM Ca²⁺ enhanced the activity by 30%. When the 21 and 15 kDa proteins were supplemented to the particles, the Ca²⁺-effect disappeared and the rate of oxygen evolution increased to a level exceeding 1000 μmol O₂ per mg chlorophyll per h. The results indicate that the number of Ca²⁺ needed to promote a high rate of oxygen evolution is one per PS II in higher plants.     

Membrane phosphorylation leads to the partial detachment of the chlorophyll a/b protein from Photosystem II

The hypothesis that the chlorophyll fluorescence decline due to membrane phosphorylation is caused principally by the detachment and removal of LHCP from the LHCP-PS II matrix is examined. It is demonstrated that when membranes are phosphorylated in the dark (a) the fluorescence decline is greater when excited by light enriched in wavelengths absorbed mainly by LHCP (475 nm) than when excited by light absorbed to a large extent also by the PS II complex (435 nm), (b) titration with different artificial quenchers of chlorophyll fluorescence is unchanged after the phosphorylation-induced fluorescence decline, and (c) the F_v/F_m ratio does not change after the phosphorylation-induced fluorescence decline. These data indicate that it is indeed principally LHCP that interacts with the quencher (PS I presumably). This interaction involves a small fraction of the total PS II-coupled LHCP, which becomes functionally detached from the LHCP-PS II matrix.     

ApcD is necessary for efficient energy transfer from phycobilisomes to photosystem I and helps to prevent photoinhibition in the cyanobacterium Synechococcus sp. PCC 7002

Phycobilisomes (PBS) are the major light-harvesting, protein-pigment complexes in cyanobacteria and red algae. PBS absorb and transfer light energy to photosystem (PS) II as well as PS I, and the distribution of light energy from PBS to the two photosystems is regulated by light conditions through a mechanism known as state transitions. In this study the quantum efficiency of excitation energy transfer from PBS to PS I in the cyanobacterium Synechococcus sp. PCC 7002 was determined, and the results showed that energy transfer from PBS to PS I is extremely efficient. The results further demonstrated that energy transfer from PBS to PS I occurred directly and that efficient energy transfer was dependent upon the allophycocyanin-B alpha subunit, ApcD. In the absence of ApcD, cells were unable to perform state transitions and were trapped in state 1. Action spectra showed that light energy transfer from PBS to PS I was severely impaired in the absence of ApcD. An apcD mutant grew more slowly than the wild type in light preferentially absorbed by phycobiliproteins and was more sensitive to high light intensity. On the other hand, a mutant lacking ApcF, which is required for efficient energy transfer from PBS to PS II, showed greater resistance to high light treatment. Therefore, state transitions in cyanobacteria have two roles: (1) they regulate light energy distribution between the two photosystems; and (2) they help to protect cells from the effects of light energy excess at high light intensities.     

Excitation energy transfer from phycobiliprotein to chlorophyll d in intact cells of Acaryochloris marina studied by time- and wavelength-resolved fluorescence spectroscopy.

The fluorescence decay spectra and the excitation energy transfer from the phycobiliproteins (PBP) to the chlorophyll-antennae of intact cells of the chlorophyll (Chl) d-dominated cyanobacterium Acaryochloris marina were investigated at 298 and 77 K by time- and wavelength-correlated single photon counting fluorescence spectroscopy. At 298 K it was found that (i) the fluorescence dynamics in A. marina is characterized by two emission peaks located at about 650 and 725 nm, (ii) the intensity of the 650 nm fluorescence depends strongly on the excitation wavelength, being high upon excitation of phycobiliprotein (PBP) at 632 nm but virtually absent upon excitation of chlorophyll at 430 nm, (iii) the 650 nm fluorescence band decayed predominantly with a lifetime of 70 +/- 20 ps, (iv) the 725 nm fluorescence, which was observed independent of the excitation wavelength, can be described by a three-exponential decay kinetics with lifetimes depending on the open or the closed state (F(0) or F(m)) of the reaction centre of Photosystem II (PS II). Based on the results of this study, it is inferred that the excitation energy transfer from phycobiliproteins to Chl d of PS II in A. marina occurs with a time constant of about 70 ps, which is about three times faster than the energy transfer from the phycobilisomes to PS II in the Chl a-containing cyanobacterium Synechococcus 6301. A similar fast PBP to Chl d excitation energy transfer was also observed at 77 K. At 77 K a small long-lived fluorescence decay component with a lifetime of 14 ns was observed in the 640-700 nm spectral range. However, it has a rather featureless spectrum, not typical for Chl a, and was only observed upon excitation at 400 nm but not upon excitation at 632 and 654 nm. Thus, this long-lived fluorescence component cannot be used as an indicator that the primary PS II donor of Acaryochloris marina contains Chl a.     

Structural organization of the oxidizing side of photosystem II. Exogenous reductants reduce and destroy the Mn-complex in photosystems II membranes depleted of the 17 and 23 kDa polypeptides

Removal of 23 and 17 kDa water-soluble polypeptides from PS II membranes causes a marked decrease in oxygen-evolution activity, exposes the oxidizing side of PS II to exogenous reductants (Ghanotakis, D.F., Babcock, G.T. and Yocum, C.F. (1984) Biochim. Biophys. Acta 765, 388–398) and alters a high-affinity binding site for Ca²⁺ in the oxygen-evolving complex (Ghanotakis, D.F., Topper, J.N., Babcock, G.T. and Yocum, C.F. (1984) FEBS Lett. 170, 169–173). We have examined further the state of the functional Mn complex in PS II membranes from which the 17 and 23 kDa species have been removed by high-salt treatment. These membranes contain a structurally altered Mn complex which is sensitive to destruction by low concentrations of NH₂OH which cannot, in native PS II membranes, cause extraction of functional Mn. In addition to NH₂OH, a wide range of other small (H₂O₂, NH₂NH₂, Fe²⁺) and bulky (benzidine, hydroquinone) electron donors extract Mn (up to 80%) from the polypeptide-depleted PS II preparations. This extraction is due to reduction of the functional Mn complex since light, which would generate higher oxidation states within the Mn complex, prevents Mn release by reductants. Release of Mn by reductants does not extract the 33 kDa water-soluble protein implicated in Mn binding to the oxidizing side of PS II, although the protein can be partially or totally extracted from Mn-depleted preparations by exposure to high ionic strength or to high (0.8 M) concentrations of Tris. We view our results as evidence for a shield around the Mn complex of the oxygen-evolving complex comprised of the 33 kDa polypeptide along with the 23 and 17 kDa proteins and tightly bound Ca²⁺.     

Specificity of energy transfer to photosystem II by in vitro reassociated homologous and heterologous membrane-bound phycobilisomes

In a previous publication we have reported the in vitro reassociation of phycobiliproteins with thylakoids of Fremyella diplosiphon to form homologous, functional, membrane-bound phycobilisomes (Kirilovsky, D., Kessel, M. and Ohad, I (1983) Biochim. Biophys. Acta 724, 416–426). In the present work, using the same experimental system, we demonstrate the in vitro formation of heterologous, membrane-bound phycobilisomes. Analysis of phycobiliprotein association and binding curves disclosed two types of binding sites: specific sites which allow energy transfer to Photosystem II and non-specific sites which become occupied only after saturation of the Photosystem II specific sites. Binding to non-specific sites does not result in energy transfer. Both types of sites are present on cyanophyte thylakoids. Thylakoids of eukaryotic chloroplasts such as those of Chlamydomonas reinhardtii or Euglena gracilis can bind phycobiliproteins which reassociate to form intact membrane-bound phycobilisomes. However, only non-specific binding occurs in such heterologous systems. Limited proteolysis of membrane-bound phycobilisomes results in a rapid loss of the 94–95 kDa polypeptide assumed to be required for binding and energy transfer (Redlinger, T. and Gantt, E. (1982) Proc. Natl. Acad. Sci. USA 79, 5542–5546). Phycobilisomes lacking this polypeptide cannot bind to either specific or non-specific sites. Based on these results, we conclude that the 94–95 kDa polypeptide is required for the association of the phycobilisomes to both homologous and heterologous membranes; however, additional factors within the Photosystem II unit of cyanophytes are also required for establishing energy transfer.     

Electrogenic reduction of the primary electron donor P700 by plastocyanin in photosystem I complexes

An electrometric technique was used to investigate electron transfer between spinach plastocyanin (Pc) and photooxidized primary electron donor P700 in photosystem I (PS I) complexes from the cyanobacterium Synechocystis sp. PCC 6803. In the presence of Pc, the fast unresolvable kinetic phase of membrane potential generation related to electron transfer between P700 and the terminal iron–sulfur acceptor F_B was followed by additional electrogenic phases in the microsecond and millisecond time scales, which contribute approximately 20% to the overall electrogenicity. These phases are attributed to the vectorial electron transfer from Pc to the protein-embedded chlorophyll dimer P700⁺ within the PsaA/PsaB heterodimer. The observed rate constant of the millisecond kinetic phase exhibited a saturation profile at increasing Pc concentration, suggesting the formation of a transient complex between Pc and PS I with the dissociation constant K_d of about 80 μM. A small but detectable fast electrogenic phase was observed at high Pc concentration. The rate constant of this phase was independent of Pc concentration, indicating that it is related to a first-order process.     

Transfer and trapping of excitation energy in Photosystem II as studied by chlorophyll a2 fluorescence quenching by dinitrobenzene and carotenoid triplet. The matrix model

1. The curves representing the reciprocal fluorescence yield of chlorophyll a of Photosystem II (PS II) in Chlorella vulgaris as a function of the concentration of m-dinitrobenzene in the states P Q and P Q^-, are found to be straight parallel lines; P is the primary donor and Q the primary acceptor of PS II. In the weakly trapping state P Q^- the half-quenching of dinitrobenzene is about 0.2 mM, in vitro it is of the order of 10 mM. The fluorescence yield as a function of the concentration of a quencher is described for three models for the structure of pigment systems: the model of separate units, the model of limited energy transfer between the units, and the matrix model. If it is assumed that the rate constant of quenching by dinitrobenzene is high and thus the number of dinitrobenzene molecules per reaction center low, it can be concluded that the pigment system of PS II in C. vulgaris is a matrix of chlorophyll molecules in which the reaction centers are embedded. Theoretical and experimental evidence is consistent with such an assumption.

For Cyanidium caldarium the zero fluorescence yield Ф₀ and its quenching by dinitrobenzene were found to be much smaller than the corresponding quantities for C. vulgaris. Nevertheless, our measurements on C. caldarium could be interpreted by the assumption that the essential properties (rate constants, dinitrobenzene quenching) of PS II are the same for these two species belonging to such widely different groups.

2. The measured dinitrobenzene concentrations required for half-quenching in vivo and other observations are explained by (non-rate-limiting) energy transfer between the chlorophyll a molecules of PS II and by the assumptions that dinitrobenzene is approximately distributed at random in the membrane and does not diffuse during excitation.

3. The fluorescence kinetics of C. vulgaris during a 350 ns laser flash of variable intensity could be simulated on a computer using the matrix model. From the observed fluorescence quenching by the carotenoid triplet (C^T) and the measurement of the number of C^T per reaction center via difference absorption spectroscopy, the rate constant for quenching of C^T is calculated to be k_T = 3.3 · 10¹¹ s⁻¹ which is almost equal to the rate constant of trapping by an open reaction center (Duysens, L.N.M. (1979) CIBA Foundation Symposium 61 (New Series), pp. 323–340).

4. The fluorescence quenching by C^T in non-treated spinach chloroplasts after a 500 ns laser flash (Breton, J., Geacintov, N.E. and Swenberg, C.E. (1979) Biochim. Biophys. Acta 548, 616–635) could be explained within the framework of the matrix model when the value for k_T is used as given in point 3.

5. The observations mentioned under point 1 indicate that the fluorescence yield Ф₀ for centers in trapping state P Q is probably for a fraction exceeding 0.8 emitted by PS II.