Steady-state polarized light spectroscopy of isolated Photosystem I complexes

Monomeric and trimeric Photosystem I core complexes from the cyanobacterium Synechocystis PCC 6803 and LHC-I containing Photosystem I (PS I-200) complexes from spinach have been characterized by steady-state, polarized light spectroscopy at 77 K. The absorption spectra of the monomeric and trimeric core complexes from Synechocystis were remarkably similar, except for the amplitude of a spectral component at long wavelength, which was about twice as large in the trimeric complexes. This spectral component did not contribute significantly to the CD-spectrum. The (77 K) steady-state emission spectra showed prominent peaks at 724 nm (for the Synechocystis core complexes) and at 735 nm (for PS I-200). A comparison of the excitation spectra of the main emission band and the absorption spectra suggested that a significant part of the excitations do not pass the red pigments before being trapped by P-700. Polarized fluorescence excitation spectra of the monomeric and trimeric core complexes revealed a remarkably high anisotropy (0.3) above 705 nm. This suggested one or more of the following possibilities: 1) there is one red-most pigment to which all excitations are directed, 2) there are more red-most pigments but with (almost) parallel orientations, 3) there are more red-most pigments, but they are not connected by energy transfer. The high anisotropy above 705 nm of the trimeric complexes indicated that the long-wavelength pigments on different monomers are not connected by energy transfer. In contrary to the Synechocystis core complexes, the anisotropy spectrum of the LHC I containing complexes from spinach was not constant in the region of the long-wavelength pigments, and decreased significantly below 720 nm, the wavelength where the long-wavelength pigments on the core complexes start to absorb. These results suggested that in spinach the long-wavelength pigments on core and LHC-I are connected by energy transfer and have a non-parallel average Q_y(0-0) transitions.Abbreviations PS Photosystem - P Primary donor - Chl chlorophyll - LHC light-harvesting complex - CD circular dichroism - LD linear dichroism - BisTris 2-[bis(2-hydroxyethyl)amino]-2-hydroxy-methylpropane-1,3-diol - RC reaction center     

Pigment and protein composition of reconstituted light-harvesting complexes and effects of some protein modifications

The structure and heterogeneity of LHC II were studied by in vitro reconstitution of apoproteins with pigments (Plumley and Schmidt 1987, Proc Natl Acad Sci 84: 146–150). Reconstituted CP 2 complexes purified by LDS-PAGE were subsequently characterized and shown to have spectroscopic properties and pigment-protein compositions and stoichiometries similar to those of authentic complexes. Heterologous reconstitutions utilizing pigments and light-harvesting proteins from spinach, pea and Chlamydomonas reinhardtii reveal no evidence of specialized binding sites for the unique C. reinhardtii xanthophyll loroxanthin: lutein and loroxanthin are interchangeable for in vitro reconstitution. Proteins modified by the presence of a transit peptide, phosphorylation, or proteolytic removal of the NH₂-terminus could be reconstituted. Evidence suggests that post-translational modification are not responsible for the presence of six electrophoretic variants of C. reinhardtii CP 2. Reconstitution is blocked by iodoacetamide pre-treatment of the apoproteins suggesting a role for cysteine in pigment ligation and/or proper folding of the pigment-protein complex. Finally, no effect of divalent cations on pigment reassembly could be detected.Abbreviations cab chlorophyll a/b-binding protein genes - Chl chlorophyll - CP2 light-harvesting chlorophyll A+b-protein complex fractionated by mildly denaturing LDS-PAGE from Photosystem II in thylakoids - CP 43 and CP 47 chlorophyll a-antenna complexes fractionated from Photosystem II in thylakoids by mildly denaturing LDS-PAGE at 4°C - IgG gamma immunoglobulin - LDS lithium dodecyl sulfate - LDS-PAGE lithium dodecyl sulfate polyacrylamide gel electrophoresis at 4°C - LHC I and LHC II thylakoid light-harvesting chlorophyll a+b-protein holocomplexes associated with Photosystems I and II, respectively - PS II Photosystem II - TX100 Triton X-100 - TX100-derived LHC light-harvesting complexes enriched in LHC II following fractionation of thylakoids by TX100     

Carotenoid distribution and deepoxidation in thylakoid pigment-protein complexes from cotton leaves and bundle-sheath cells of maize

In response to excess light, the xanthophyll violaxanthin (V) is deepoxidized to zeaxanthin (Z) via antheraxanthin (A) and the degree of this deepoxidation is strongly correlated with dissipation of excess energy and photoprotection in PS II. However, little is known about the site of V deepoxidation and the localization of Z within the thylakoid membranes. To gain insight into this problem, thylakoids were isolated from cotton leaves and bundle-sheath strands of maize, the pigment protein-complexes separated on Deriphat gels, electroeluted, and the pigments analyzed by HPLC. In cotton thylakoids, 30% of the xanthophyll cycle pigments were associated with the PS I holocomplex, including the PS I light-harvesting complexes and PS I core complex proteins (CC I), and about 50% with the PS II light-harvesting complexes (LHC II). The Chl was evenly distributed between PS I and PS II. Less than 2% of the neoxanthin, about 18% of the lutein, and as much as 76% of the -carotene of the thylakoids were associated with PS I. Exposure of pre-darkened cotton leaves to a high photon flux density for 20 min prior to thylakoid isolation caused about one-half of the V to be converted to Z. The distribution of Z among the pigment-protein complexes was found to be similar to that of V. The distribution of the other carotenoids was unaffected by the light treatment. Similarly, in field-grown maize leaves and in the bundle-sheath strands isolated from them, about 40% of the V present at dawn had been converted to Z at solar noon. Light treatment of isolated bundle-sheath strands which initially contained little Z caused a similar degree of conversion of V to Z. As in cotton thylakoids, about 30% the V+A+Z pool in bundle-sheath thylakoids from maize was associated with the PS I holocomplex and the CC I bands and 46% with the LHC II bands, regardless of the extent of deepoxidation. These results demonstrate that Z is present in PS I as well as in PS II and that deepoxidation evidently takes place within the pigment-protein complexes of both photosystems.Abbreviations A antheraxanthin - CC I, CC II Core or reaction center complex of PS I, PS II - CP Chl protein - EPS epoxidation state - F_m Chl fluorescence at closed PS II reaction centers - IEF isoelectric focussing gels - LHC I, LHC II light-harvesting complex of PS I, PS II - OE oxygen evolving polypeptide - PFD photon flux density - PS I^* PS I holocomplex - V violaxanthin - Z zeaxanthin - antibody against C.I.W.-D.P.B. Publication No. 1127.     

Organization of chlorophyll-protein complexes of Photosystem I in Chlamydomonas reinhardii

The polypeptide pattern, chlorophyll-protein complexes, fluorescence emission spectra and light intensity required for saturation of electron flow via Photosystem (PS) II and PS I in a pale-green photoautotrophic mutant, y-lp, were compared to those of the parent strain, Chlamydomonas reinhardii y-1 cells. The mutant exhibits a 686 nm fluorescence yield at 25°C and 77 K 2–6-fold higher than that of the parent strain cells, and is deficient in thylakoid polypeptides 14, 17.2, 18 and 22 according to the nomenclature of Chua (Chua, N.-H. (1980) Methods Enzymol. 60C, 434–446). All chlorophyll-protein complexes ascribed to PS II and the CP I complex were present in both type of cells. However, a chlorophyll-protein complex CP Ia containing — in the parent strain — the 66–68 kDa polypeptides of CP I and the four above-mentioned polypeptides, was absent in the mutant. It was previously reported that a chlorophyll-protein complex, CP O, obtained from C. reinhardii contains five polypeptides, namely, 14, 15, 17.2, 18 and 22 (Wollman, F.A. and Bennoun, P. (1982) Biochim. Biophys. Acta 680, 352–360). A CP O-like complex was present also in the mutant y-lp cells but it contains only one polypeptide, 15. Energy transfer from PS II to PS I was not impaired in the mutant, although a 4-fold higher light intensity was required for the saturation of PS I electron flow in the y-lp cells as compared with the parent strain. No difference was found in the light saturation curves for PS II activity between the mutant and parent strain cells. Based on these and additional data (Gershoni, J.M., Shochat, S., Malkin, S. and Ohad, I. (1982) Plant Physiol. 70, 637–644), it is concluded that the chlorophyll-protein complexes of PS I in Chlamydomonas comprise a reaction center-core antenna complex containing the 66–68 kDa polypeptides (CP I), a connecting antenna consisting of four polypeptides (14, 17.2, 18 and 22), and a light-harvesting antenna containing one polypeptide, 15. These appear to be organized as a complex, CP Ia. The interconnecting antenna is deficient in the y-lp mutant and thus the CP Ia complex is unstable and energy is not transferred from CP O to CP I. The effective cross-section of PS I antenna is thus reduced and a high fluorescence is emitted at 686 nm.     

Light-Harvesting Features Revealed by the Structure of Plant Photosystem I

Oxygenic photosynthesis is driven by two multi-subunit membrane protein complexes, Photosystem I and Photosystem II. In plants and green algae, both complexes are composed of two moieties: a reaction center (RC), where light-induced charge translocation occurs, and a peripheral antenna that absorbs light and funnels its energy to the reaction center. The peripheral antenna of PS I (LHC I) is composed of four gene products (Lhca 1-4) that are unique among the chlorophyll a/b binding proteins in their pronounced long-wavelength absorbance and in their assembly into dimers. The recently determined structure of plant Photosystem I provides the first relatively high-resolution structural model of a super-complex containing a reaction center and its peripheral antenna. We describe some of the structural features responsible for the unique properties of LHC I and discuss the advantages of the particular LHC I dimerization mode over monomeric or trimeric forms. In addition, we delineate some of the interactions between the peripheral antenna and the reaction center and discuss how they serve the purpose of dynamically altering the composition of LHC I in response to environmental pressure. Combining structural insight with spectroscopic data, we propose how altering LHC I composition may protect PS I from excessive light.     

Structural and functional organization of the peripheral light-harvesting system in Photosystem I

This review centers on the structural and functional organization of the light-harvesting system in the peripheral antenna of Photosystem I (LHC I) and its energy coupling to the Photosystem I (PS I) core antenna network in view of recently available structural models of the eukaryotic Photosystem I–LHC I complex, eukaryotic LHC II complexes and the cyanobacterial Photosystem I core. A structural model based on the 3D homology of Lhca4 with LHC II is used for analysis of the principles of pigment arrangement in the LHC I peripheral antenna, for prediction of the protein ligands for the pigments that are unique for LHC I and for estimates of the excitonic coupling in strongly interacting pigment dimers. The presence of chlorophyll clusters with strong pigment–pigment interactions is a structural feature of PS I, resulting in the characteristic red-shifted fluorescence. Analysis of the interactions between the PS I core antenna and the peripheral antenna leads to the suggestion that the specific function of the red pigments is likely to be determined by their localization with respect to the reaction center. In the PS I core antenna, the Chl clusters with a different magnitude of low energy shift contribute to better spectral overlap of Chls in the reaction center and the Chls of the antenna network, concentrate the excitation around the reaction center and participate in downhill enhancement of energy transfer from LHC II to the PS I core. Chlorophyll clusters forming terminal emitters in LHC I are likely to be involved in photoprotection against excess energy.     

Excitation energy transfer in Photosystem I from oxygenic organisms

This Review discusses energy transfer pathways in Photosystem I (PS I) from oxygenic organisms. In the trimeric PS I core from cyanobacteria, the efficiency of solar energy conversion is largely determined by ultrafast excitation transfer processes in the core chlorophyll a (Chl a) antenna network and efficient photochemical trapping in the reaction center (RC). The role of clusters of Chl a in energy equilibration and photochemical trapping in the PS I core is discussed. Dimers of the longest-wavelength absorbing (red) pigments with strongest excitonic interactions localize the excitation in the PS I core antenna. Those dimers that are located closer to the RC participate in a fast energy equilibration with coupled pigments of the RC. This suggests that the function of the red pigments is to concentrate the excitation near the RC. In the PS I holocomplex from algae and higher plants, in addition to the red pigments of the core antenna, spectrally distinct red pigments are bound to the peripheral Chl a/b-binding light-harvesting antenna (LHC I), specifically to the Lhca4 subunit of the LHC I-730 complex. Intramonomeric energy equilibration between pools of Chl b and Chl a in Lhca1 and Lhca4 monomers of the LHC I-730 heterodimer are as fast as the energy equilibration processes within the PS I core. In contrast to the structural stability of the PS I core, the flexible subunit structure of the LHC I would probably determine the observed slow excitation energy equilibration processes in the range of tens of picoseconds. The red pigments in the LHC I are suggested to function largely as photoprotective excitation sinks in the peripheral antenna of PS I. This revised version was published online in August 2006 with corrections to the Cover Date.     

Identification of Photosystem I components from a glaucocystophyte,Cyanophora paradoxa: The PsaD protein has an N-terminal stretch homologous to higher plants

Thylakoid membranes and Photosystem I (PS I) complexes were isolated from a glaucocystophyte, Cyanophora paradoxa, which is thought to have the most primitive ‘plastids’, and the proteins related to PS I were examined. The intrinsic light-harvesting chlorophyll protein complexes of PS I (LHC I) were not detected by an immunological method. The PS I complexes consisted of at least eight low-molecular-mass proteins in addition to PS I reaction center proteins. The N-terminal sequence of the PsaD protein has higher homology to that of Chlamydomonas reinhardtii and land plants, than to that of other algae or cyanobacteria. On the other hand, the PsaL sequence has the highest homology to those of cyanobacteria. Taking into account the other sequences of PS I components whose genes are encoded in the cyanelle genome, and the fact that LHC I is not detected, it is concluded that PS I of C. paradoxa has chimeric characteristics of both ‘green’ lineages and cyanobacteria. This revised version was published online in June 2006 with corrections to the Cover Date.     

A new chlorophyll-protein complex related to Photosystem I in Chlamydomonas reinhardii

A new chlorophyll-protein complex, CP O, was isolated from Chlamydomonas reinhardii using lithium dodecyl sulfate polyacrylamide gel electrophoresis run at 4°C. A similar complex is recovered using Triton/digitonin solubilization of thylakoid membranes of the F54-14 mutant lacking in CP I and ATPase. CP O is enriched in long-wavelength chlorophyll a and contains five polypeptides (27.5, 27, 25, 23 and 19 kDa). Its 77 K fluorescence emission spectrum peaks at 705 nm while CP II have an emission maximum at 682 and 720 nm, respectively. Comparison of the polypeptide pattern of the wild type and AC40 mutant of C. reinhardii shows that the five CP O polypeptides are specifically lacking in the mutant. Although the 77 K emission originating from the Photosystem (PS) I pigments is lower in the mutant than in the wild type, the two spectra show the same peaks at 686, 694 and 717 nm. However, comparison of the 77 K emission spectrum of the F14 mutant lacking in CP I with that of the double mutant AC40-14 lacking in CP I and CP O shows the absence in the latter of the large emission band peaking at 707 nm. The 707 nm emission is thought to arise from some PS I antennae and is quenched in the wild type by the presence of PS I traps located in CP I. We conclude that CP O is a part of the PS I antenna in C. reinhardii which controls the 707 nm fluorescence emission.     

Development of Photosystem II in dark grown Chlamydomonas reinhardtii. A light-dependent conversion of PS IIβ, QB-nonreducing centers to the PS IIα, QB-reducing form

The green alga Chlamydomonas reinhardtii is a facultative heterotroph and, when cultured in the presence of acetate, will synthesize chlorophyll (Chl) and photosystem (PS) components in the dark. Analysis of the thylakoid membrane composition and function in dark grown C. reinhardtii revealed that photochemically competent PS II complexes were synthesized and assembled in the thylakoid membrane. These PS II centers were impaired in the electron-transport reaction from the primary-quinone electron acceptor, Q_A, to the secondary-quinone electron acceptor, Q_B (Q_B-nonreducing centers). Both complements of the PS II Chl a–b light harvesting antenna (LHC II-inner and LHC II-peripheral) were synthesized and assembled in the thylakoid membrane of dark grown C. reinhardtii cells. However, the LHC II-peripheral was energetically uncoupled from the PS II reaction center. Thus, PS II units in dark grown cells had a -type Chl antenna size with only 130 Chl (a and b) molecules (by definition, PS II units lack LHC II-peripheral). Illumination of dark grown C. reinhardtii caused pronounced changes in the organization and function of PS II. With a half-time of about 30 min, PS II centers were converted froma Q_B-nonreducing form in the dark, to a Q_B-reducing form in the light. Concomitant with this change, PS II units were energetically coupled with the LHC II-peripheral complement in the thylakoid membrane and were converted to a PS II form. The functional antenna of the latter contained more than 250 Chl(a+b) molecules. The results are discussed in terms of a light-dependent activation of the Q_A-Q_B electron-transfer reaction which is followed by association of the PS II unit with a LHC II-peripheral antenna and by inclusion of the mature form of PS II (PS II) in the membrane of the grana partition region.Abbreviations Chl chlorophyll - PS photosystem - Q_A primary quinone electron acceptor of PS II - Q_B secondary quinone electron acceptor of PS II - LHC light harvesting complex - F₀ non-variable fluorescence yield - F_plf intermediate fluorescence yield plateau leyel - F_max maximum fluorescence yield - F_i initial fluorescence yield increase from F₀ to F_pl (F_pl–F₀) - F_v total variable fluorescence yield (F_m–F0) - DCMU dichlorophenyl-dimethylurea     

Orientation of pigments in the thylakoid membrane and in the isolated chlorophyll-protein complexes of higher plants. II. Linear dichroism spectra of isolated pigment-protein complexes oriented in polyacrylamide gels at 300 and 100 K

The absorption and linear dichroism (LD) spectra (380–780 nm) of isolated light-harvesting complex (LHC), Photosystem I (PS I), Photosystem II (PS II), as well as intact thylakoids have been determined at 300 and 100 K. The samples were oriented in squeezed polyacrylamide gel. The low-temperature spectra of LHC and PS I present LD signals which are characteristic enough to be recognized in the LD spectrum of thylakoids. Tentative assignments of the various features of the LD spectra to the major photosynthetic pigments are discussed. A shoulder in the low-temperature absorption spectra is observed at about 673 nm in all the systems under investigation. The absence of an associated LD signal suggests that this ubiquitous chlorophyll (Chl) a form is non-dichroic. Furthermore, in the three isolated chlorophyll-protein complexes described in this study the sign of the LD signal indicates that both the Q_y transition of the Chl a and the carotenoid molecules are preferentially oriented parallel to the largest dimension(s) of the particles.     

Light-harvesting chlorophyll a-b complex requirement for regulation of Photosystem II photochemistry by non-photochemical quenching

Recently, it has been suggested (Horton et al. 1992) that aggregation of the light-harvesting a-b complex (LHC II) in vitro reflects the processes which occur in vivo during fluorescence induction and related to the major non-photochemical quenching (qE). Therefore the requirement of this chlorophyll a-b containing protein complex to produce qN was investigated by comparison of two barley mutants either lacking (chlorina f2) or depressed (chlorina¹⁰⁴) in LHC II to the wild-type and pea leaves submitted to intermittent light (IL) and during their greening in continuous light. It was observed that qN was photoinduced in the absence of LHC II, i.e. in IL grown pea leaves and the barley mutants. Nevertheless, in these leaves qN had no (IL, peas) or little (barley mutants) inhibitory effect on the photochemical efficiency of Q_A reduction measured by flash dosage response curves of the chlorophyll fluorescence yield increase induced by a single turn-over flash During greening in continuous light of IL pea leaves, an inhibitory effect on Q_A photoreduction associated to qN developed as Photosystem II antenna size increased with LHC II synthesis. Utilizing data from the literature on connectivity between PS II units versus antenna size, the following hypothesis is put forward to explain the results summarized above. qN can occur in the core antenna or Reaction Center of a fraction of PS II units and these units will not exhibit variable fluorescence. Other PS II units are quenched indirectly through PS II-PS II exciton transfer which develops as the proportion of connected PS II units increases through LHC II synthesis.     

Kinetics of excitation trapping in intact Photosystem I of Chlamydomonas reinhardtii and Arabidopsis thaliana

We measured picosecond time-resolved fluorescence of intact Photosystem I complexes from Chlamydomonas reinhardtii and Arabidopsis thaliana. The antenna system of C. reinhardtii contains about 30-60 chlorophylls more than that of A. thaliana, but lacks the so-called red chlorophylls, chlorophylls that absorb at longer wavelength than the primary electron donor. In C. reinhardtii, the main lifetimes of excitation trapping are about 27 and 68 ps. The overall lifetime of C. reinhardtii is considerably shorter than in A. thaliana. We conclude that the amount and energies of the red chlorophylls have a larger effect on excitation trapping time in Photosystem I than the antenna size.     

Structure and composition of the photochemical apparatus of the antarctic green alga,Chlamydomonas subcaudata

The green alga, Chlamydomonas subcaudata, collected from a perennially ice-covered Antarctic lake, was able to grow at temperatures of 16°C or lower, but not at temperatures of 20°C or higher, which confirmed its psychrophilic nature. Low temperature (77 K) Chl a fluorescence emission spectra of whole cells of the mesophile, C. reinhardtii, indicated the presence of major emission bands at 681 and 709 nm associated with PS II and PS I, respectively. In contrast, emission spectra of whole cells of C. subcaudata exhibited major emission bands at 681 and 692 nm associated with PS II, but the absence of a major PS I emission band at 709 nm. These results for C. subcaudata were consistent with: (1) low ratio of Chl a/b (1.80); (2) low levels of PsaA/PsaB heterodimer as well as specific Lhca polypeptides as determined by immunoblotting, (3) decreased levels of the Chl-protein complexes CP1 and LHC I associated with PS I; and (4) an increased stability of the oligomeric form of LHC II as assessed by non-denaturing gel electrophoresis in the psychrophile compared to the mesophile. Furthermore, immunoblotting indicated that the stoichiometry of PS II:PS I:CF₁ is significantly altered in C. subcaudata compared to the mesophile. Even though the psychrophile is adapted to growth at low irradiance, it retained the capacity to adjust the total xanthophyll cycle pool size as well as the epoxidation state of the xanthophyll cycle. Despite these differences, the psychrophile and mesophile exhibited comparable photosynthetic efficiency for O₂ evolution regardless of growth conditions. P^max for both Chlamydomonas species was similar only when grown under identical conditions. We suggest that these photosynthetic characteristics of the Antarctic psychrophile reflect the unusual light and low temperature regime to which it is adapted.     

Antenna function of a chlorophyll ab protein complex of Photosystem I

The functional role of a chlorophyll $\text{a}\text{b}$ complex associated with Photosystem I (PS I) has been studied. The rate constant for P-700 photooxidation, K_P-700, which under light-limiting conditions is directly proportional to the size of the functional light-harvesting antenna, has been measured in two PS I preparations, one of which contains the chlorophyll $\text{a}\text{b}$ complex and the other lacking the complex. K_P-700 for the former preparation is half of that of the preparation which has the chlorophyll $\text{a}\text{b}$ complex present. This difference reflects a decrease in the functional light-harvesting antenna in the PS I complex devoid of the chlorophyll $\text{a}\text{b}$ complex. Experiments involving reconstitution of the chlorophyll $\text{a}\text{b}$ complex with the antenna-depleted PS I preparation indicate a substantial recovery of the K_P-700 rate. These results demonstrate that the chlorophyll $\text{a}\text{b}$ complex functions as a light-harvesting antenna in PS I.     

The PsbP Domain Protein 1 Functions in the Assembly of Lumenal Domains in Photosystem I

Photosystem I (PS I) is a multisubunit membrane protein complex that functions as a light-driven plastocyanin-ferredoxin oxidoreductase. The PsbP domain protein 1 (PPD1; At4g15510) is located in the thylakoid lumen of plant chloroplasts and is essential for photoautotrophy, functioning as a PS I assembly factor. In this work, RNAi was used to suppress PPD1 expression, yielding mutants displaying a range of phenotypes with respect to PS I accumulation and function. These PPD1 RNAi mutants showed a loss of assembled PS I that was correlated with loss of the PPD1 protein. In the most severely affected PPD1 RNAi lines, the accumulated PS I complexes exhibited defects in electron transfer from plastocyanin to the oxidized reaction center P₇₀₀⁺. The defects in PS I assembly in the PPD1 RNAi mutants also had secondary effects with respect to the association of light-harvesting antenna complexes to PS I. Because of the imbalance in photosystem function in the PPD1 RNAi mutants, light-harvesting complex II associated with and acted as an antenna for the PS I complexes. These results provide new evidence for the role of PPD1 in PS I biogenesis, particularly as a factor essential for proper assembly of the lumenal portion of the complex.     

Linear dichroism of microalgae,developing thylakoids and isolated pigment-protein complexes in stretched poly (vinyl alcohol) films at 77 K

A variety of unicellular algae, thylakoids from higher plants in different stages of maturity and isolated pigment-protein complexes were oriented in stretched polyvinyl alcohol films. Low temperature linear dichroism (LD) spectra of Chlorella pyrenoidosa and higher plant thylakoids in the films were very similar to those obtained after orientation of similar samples using magnetic or electric fields.Positive LD bands corresponding to Chl a (670) and (682) and negative bands due to Chl a (658) and Chl b (648) were resolved in spectra of the light harvesting Chl a/b protein. Chl b (648) and Chl a (658) and (670) were not seen in the LD spectrum of thylakoids from plants grown in intermittent light, the Chl b-less mutant of barley, Euglena gracilis or the cyanobacteria, Phormidium luridum and Anacystis nidulans, but did appear upon chloroplast maturation in Romaine lettuce and during the greening of etiolated and intermittent light plants. The highly oriented long wavelength Chl a (682) in the light-harvesting complex may represent residual PS II whose peak dichroism is centered at 681 nm. The PS I preparation had a Chl $\text{a}\text{b}$ ratio of approx. 6 and the LD spectrum was positive with a maximum at 690–694 nm and a band of lower amplitude at 652 nm. The minor LD band was not observed in PS I preparations from organisms that lack Chl b such as the cyanobacteria, intermittent light plants and the Chl b-less mutant of barley. We suggest that the 652 nm band is due to Chl b molecules associated with the antenna of PS I and are distinct from those on the light harvesting complex whose orientation is different. We also conclude that all the Chl a forms are oriented and that the long geometric axes of the pigment-protein complexes, as deduced from the configuration they assume in the stretched films, are axes that normally lie parallel to the plane of the native thylakoid.     

Solubilization of green plant thylakoid membranes with n-dodecyl-α,D-maltoside. Implications for the structural organization of the Photosystem II,Photosystem I,ATP synthase and cytochrome b6 f complexes

A biochemical and structural analysis is presented of fractions that were obtained by a quick and mild solubilization of thylakoid membranes from spinach with the non-ionic detergent n-dodecyl-α,D-maltoside, followed by a partial purification using gel filtration chromatography. The largest fractions consisted of paired, appressed membrane fragments with an average diameter of about 360 nm and contain Photosystem II (PS II) and its associated light-harvesting antenna (LHC II), but virtually no Photosystem I, ATP synthase and cytochrome b ₆ f complex. Some of the membranes show a semi-regular ordering of PS II in rows at an average distance of about 26.3 nm, and from a partially disrupted grana membrane fragment we show that the supercomplexes of PS II and LHC II represent the basic structural unit of PS II in the grana membranes. The numbers of free LHC II and PS II core complexes were very high and very low, respectively. The other macromolecular complexes of the thylakoid membrane occurred almost exclusively in dispersed forms. Photosystem I was observed in monomeric or multimeric PS I-200 complexes and there are no indications for free LHC I complexes. An extensive analysis by electron microscopy and image analysis of the CF₀F₁ ATP synthase complex suggests locations of the δ (on top of the F₁ headpiece) and ∈ subunits (in the central stalk) and reveals that in a substantial part of the complexes the F₁ headpiece is bended considerably from the central stalk. This kinking is very likely not an artefact of the isolation procedure and may represent the complex in its inactive, oxidized form. This revised version was published online in June 2006 with corrections to the Cover Date.     

High Yield Non-detergent Isolation of Photosystem I-Light-harvesting Chlorophyll II Membranes from Spinach Thylakoids: IMPLICATIONS FOR THE ORGANIZATION OF THE PS I ANTENNAE IN HIGHER PLANTS*

Styrene-maleic acid copolymer was used to effect a non-detergent partial solubilization of thylakoids from spinach. A high density membrane fraction, which was not solubilized by the copolymer, was isolated and was highly enriched in the Photosystem (PS) I-light-harvesting chlorophyll (LHC) II supercomplex and depleted of PS II, the cytochrome b₆/f complex, and ATP synthase. The LHC II associated with the supercomplex appeared to be energetically coupled to PS I based on 77 K fluorescence, P₇₀₀ photooxidation, and PS I electron transport light saturation experiments. The chlorophyll (Chl) a/b ratio of the PS I-LHC II membranes was 3.2 ± 0.9, indicating that on average, three LHC II trimers may associate with each PS I. The implication of these findings within the context of higher plant PS I antenna organization is discussed.     

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