Lateral heterogeneity in the distribution of chlorophyll-protein complexes of the thylakoid membranes of spinach chloroplasts

The lateral distribution of the main chlorophyll-protein complexes between appressed and non-appressed thylakoid membranes has been studied. The reaction centre complexes of Photosystems I and II and the light-harvesting complex have been resolved by an SDS-polyacrylamide gel electrophoretic method which permits most of the chlorophyll to remain protein-bound.

The analyses were applied to subchloroplast fractions shown to be derived from different thylakoid regions. Stroma thylakoids were separated from grana stacks by centrifugation following chloroplast disruption by press treatment or digitonin. Vesicles derived from the grana partitions were isolated by aqueous polymer two-phase partition. A substantial depletion in the amount of Photosystem I chlorophyll-protein complex and an enrichment in the Photosystem II reaction centre complex and the light-harvesting complex occurred in the appressed grana partition region. The high enrichment in this fraction compared to grana stack fractions derived from press or digitonin treatments, suggests that the grana Photosystem I is restricted mainly to the non-appressed grana end membranes and margins, and that the grana partitions possess mainly Photosystem II reaction centre complex and the light-harvesting complex.

In contrast, stroma thylakoids are highly enriched in the Photosystem I reaction centre complex. They possess also some 10–20% of the total Photosystem II reaction centre complex and the light-harvesting complex.

The ratio of light-harvesting complex to Photosystem II reaction centre complex is rather constant in all subchloroplast fractions suggesting a close association between these complexes. This was not so for the ratio of light-harvesting complex and the Photosystem I reaction centre complex.

The lateral heterogeneity in the distribution of the photosystems between appressed and non-appressed membranes must have a profound impact on current understanding of both the distribution of excitation energy and photosynthetic electron transport between the photosystems.     

Conformation and orientation of chlorophyll-proteins in photosystem I by circular dichroism and polarized infrared spectroscopies

The protein conformation and orientation of Photosystem I (PS I) particles have been investigated by a combination of ultraviolet circular dichroism and polarized infrared spectroscopies. These PS I particles have been studied before and after reconstitution in phosphatidylcholine vesicles. The native state of the pigments of PS I was characterized by monitoring the low-temperature fluorescence emission spectra as well as the visible CD and linear dichroism spectra at room temperature. Computed analysis of the ultraviolet CD spectra of PS I complex indicates that the secondary structure of the protein is largely α-helical (52 ± 4%) with a very low amount of β-structure. Polarized infrared difference spectra of oriented PS I show a significant orientation of these α-helical segments with the α-helix axes tilted on the average at approx. 35° from the membrane normal.     

Fluorescence decay kinetics of mutants of corn deficient in photosystem I and photosystem II

The fast fluorescence decay kinetics of two photosynthetic mutants of corn (Zea mays) have been compared with those of normal corn. The fluorescence of normal corn can be resolved into three exponential decay components of lifetime 900–1500 ps (slow), 300–500 ps (middle) and 50–120 ps (fast), the yields of which are affected by light intensity and Mg²⁺ levels. The Photosystem II-(PS II)-defective mutant hcf-3 has similar decay lifetimes (approx. 1200, 450 and 100 ps) but is not affected by light intensity, reflecting the absence of PS II charge recombination. However, yields do respond to Mg²⁺ in a fashion typical of normal corn, which may be correlated with the presence of normal levels of light-harvesting chlorophyll a + b complex (LHCP). The PS I mutant hcf-50 also shows three-component decay kinetics. In conjunction with the results on the LHCP-deficient mutant of barley presented in a recent paper (Karukstis, K.K. and Sauer, K. (1984) Biochim. Biophys. Acta 766, 148–155), these data suggest that the slow component of normal chloroplasts is kinetically controlled by the decay processes of the LHCP and that the energy comes from one of two sources: (a) charge recombination in the reaction centre or (b) energy transferred within or between LHCP units only. The fast component appears to originate from both PS I and PS II. The complex response of the middle component to cations and light intensity, and its presence in all of the mutants, suggests that it also may have multiple origins.     

Energy transfer in the photochemical apparatus of flashed bean leaves

Fluorescence and energy transfer properties of bean leaves greened by brief, repetitive xenon flashes were studied at −196 °C. The bleaching of P-700 has no influence on the yield of fluorescence at any wavelength of emission. The light-induced fluorescence yield changes which are observed in both the 690 and 730 nm emission bands in the low temperature fluorescence spectra are due to changes in the state of the Photosystem II reaction centers. The fluorescence yield changes in the 730 nm band are attributed to energy transfer from Photosystem II to Photosystem I. Such energy transfer was also confirmed by measurements of the rate of photooxidation of P-700 at −196 °C in leaves in which the Photosystem II reaction centers were either all open or all closed. It is concluded that energy transfer from Photosystem II to Photosystem I occurs in the flashed bean leaves which lack the light-harvesting chlorophyll a/b protein.     

The fractionation of plant photoactive pigment-protein complexes I and II

The pigment-protein complexes enriched with Photosystem I (PPC-I) and Photosystem II (PPC-II) were obtained using sievorptive chromatography on DEAE-Sephadex column. Both types of complexes contain Chlorophyll a, β-carotene and minor quantities of Chl b. Red absorbance maxima are located at 676 nm and 673 nm for PPC-I and PPC-II, respectively. The degrees of reaction centre enrichment were measured by the method of differential spectrophotometry: PPC-I has one P-700 per 35 bulk Chl a molecules, PPC-II contains one P-680 per 18 bulk Chl a molecules. The yield of PPC-II is 7–10 times lower than that of PPC-I. After one chromatographic procedure the amount of P-680 in PPC-I preparation does not exceed 7% of that of P-700, the amount of P-700 in PPC-II preparation 2% of that of P-680. The product of PPC-II degradation was studied.     

Excitation spectra for Photosystem I and Photosystem II in chloroplasts and the spectral characteristics of the distribution of quanta between the two photosystems

The parameters listed in the title were determined within the context of a model for the photochemical apparatus of photosynthesis.

The fluorescence of variable yield at 750 nm at −196 °C is due to energy transfer from Photosystem II to Photosystem I. Fluorescence excitation spectra were measured at −196 °C at the minimum, F_O, level and the maximum, F_M, level of the emission at 750 nm. The difference spectrum, F_M–F_O, which represents the excitation spectrum for F_V is presented as a pure Photosystem II excitation spectrum. This spectrum shows a maximum at 677 nm, attributable to the antenna chlorophyll a of Photosystem II units, with a shoulder at 670 nm and a smaller maximum at 650 nm, presumably due to chlorophyll a and chlorophyll b of the light-harvesting chlorophyll complex.

Fluorescence at the F_O level at 750 nm can be considered in two parts; one part due to the fraction of absorbed quanta, , which excites Photosystem I more-or-less directly and another part due to energy transfer from Photosystem II to Photosystem I. The latter contribution can be estimated from the ratio of F_O/F_V measured at 692 nm and the extent of F_V at 750 nm. According to this procedure the excitation spectrum of Photosystem I at −196 °C was determined by subtracting 1/3 of the excitation spectrum of F_V at 750 nm from the excitation spectrum of F_O at 750 nm. The spectrum shows a relatively sharp maximum at 681 nm due to the antenna chlorophyll a of Photosystem I units with probably some energy transfer from the light-harvesting chlorophyll complex.

The wavelength dependence of was determined from fluorescence measurements at 692 and 750 nm at −196 °C. is constant to within a few percent from 400 to 680 nm, the maximum deviation being at 515 nm where shows a broad maximum increasing from 0.30 to 0.34. At wavelengths between 680 and 700 nm, increases to unity as Photosystem I becomes the dominant absorber in the photochemical apparatus.     

Chloroplast membranes of the green alga Acetabularia mediterranea. I. Isolation of the Photosystem II

1. In the presence of Triton X-100, chloroplast membranes of the green alga Acetabularia mediterranea were disrupted into two subchloroplast fragments which differed in buoyant density. Each of these fractions had distinct and unique complements of polypeptides, indicating an almost complete separation of the two fragments.

2. One of the two subchloroplast fractions was enriched in chlorophyll b. It exhibited Photosystem II activity, was highly fluorescent and was composed of particles of approx. 50 Å diameter.

3. The light-harvesting chlorophyll-protein complex of the Photosystem II-active fraction had a molecular weight of 67 000 and contained two different subunits of 23 000 and 21 500. The molecular ratio of these two subunits was 2:1.     

Isolation and properties of particles containing the reactioncenter complex of Photosystem II from spinach chloroplasts

By density gradient centrifugation of the 80000 × g supernatant of digitonintreated spinach chloroplasts two main green bands and one minor green band were obtained. The purification and properties of the particles present in the main bands, which were shown to be derived from Photosystem I and Photosystem II, have been described previously; those of the particles in the minor fraction will be described in the present paper.

After purification, these particles show Photosystem II activity but are devoid of Photosystem I activity. They have a high chlorophyll a/chlorophyll b ratio and are enriched in β-carotene and cytochrome b₅₅₉. At liquid nitrogen temperature, photoreduction of C550 and photooxidation of cytochrome-b₅₅₉ can be observed. At room temperature, cytochrome b₅₅₉ undergoes slight photooxidation.

These properties indicate that this particle may be the reaction-center complex of Photosystem II. It is suggested that, in vivo, the Photosystem II unit is made up of a reaction-center complex and an accessory complex, the latter being found in one of the main green bands of the density gradient.     

Concentration-dependent effects of salicylaldoxime on chloroplast reactions

Salicylaldoxime has been found to have a variety of concentration-dependent effects on chloroplast activities. At low concentrations (< 10 mM), salicylaldoxime reversibly inhibits all reactions which involve Photosystem II. Since the DCMU-insensitive silicomolybdate Hill reaction is also inhibited, one site of inhibition is definitely located before the DCMU-sensitive site, possibly before the photoact. The inhibition kinetics and the response of chloroplast fluorescence may indicate another site in the DCMU-sensitive region. At almost exactly the same concentrations (< 10 mM), salicylaldoxime uncouples phosphorylation reversibly, whether it is supported by Photosystem II or by Photosystem I. At higher concentrations (approx. 20 mM) salicylaldoxime inhibits Photosystem II irreversibly, uncouples irreversibly, and begins to cause changes in chloroplast light scattering which could be manifestations of membrane damage. At very high concentrations (approx. 45 mM) salicylaldoxime irreversibly inhibits Photosystem I activity in the region of plastocyanin. This is indicated by the ability of salicylaldoxime to inhibit the photooxidation of cytochrome f but not the photooxidation of P-700.     

A chlorophyll b-less mutant of Chlamydomonas reinhardii lacking in the light-harvesting chlorophyll a/b-protein complex but not in its apoproteins

The mutant pg 113, derived from Chlamydomonas reinhardii, arg₂⁻ mt⁺ (parent strain), completely lacks chlorophyll (Chl) b but is still able to grow under autotrophic conditions. The light-harvesting Chl a/b-protein complex (LHCP) is absent. This is shown (a) by the lack of the corresponding signal in the CD spectrum of thylakoids and (b) by the absence of the band of the LHCP after electrophoresis of partially solubilized thylakoid membranes on lithium dodecyl sulfate polyacrylamide gels. All the other chlorophyll-protein complexes are present. In spite of the absence of the LHCP, all the polypeptide components of this complex are present in the mutant in the same ratios as in the parent strain, although in slightly reduced amounts. The LHC apoproteins are synthesized, processed and transported into the thylakoid membrane of the mutant. Moreover, the phosphorylation of thylakoid membrane polypeptides, which is related to the regulation of the energy distribution between Photosystem I and II, is the same in the mutant and in the parent strain, indicating that phosphorylation is not dependent on the presence of Chl b. Electron micrographs of thin sections of whole cells show that there are stacked regions of thylakoids in both the mutant and the parent strain chloroplasts. However, in the mutant, stacks are located near the chloroplast envelope, while long stretches or sometimes circles of unstacked membranes are found in the interior, mostly around the pyrenoid.     

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.     

Rapid isolation of photosystem I chlorophyll-binding proteins by anion exchange perfusion chromatography

With the new method of anion exchange perfusion chromatography we have devised an extremely rapid technique to subfractionate spinach Photosystem I into its chlorophyll a containing core complex and various components of the Photosystem I light-harvesting antenna (LHC I). The isolation time for the LHC I subcomplexes following solubilisation of native Photosystem I was reduced from 50 h using traditional density centrifugation procedures down to only 10–25 min by perfusion chromatography. Within this very short period of isolation, LHC I has been obtained as subfractions highly enriched in Lhca2+3 (LHC I-680) and Lhca1+4 (LHC I-730). Moreover, other highly enriched subfractions of LHC I such as Lhca2, Lhca3 and Lhca1+2+4 were obtained where the later two populations have not previously been obtained in a soluble form and without the use of SDS. These various subfractions of the LHC I antenna have been characterised by absorption spectroscopy, 77 K fluorescence-spectroscopy and SDS-PAGE demonstrating their identities, functional intactness and purity. Furthermore, the analyses located a chlorophyll b pool to preferentially transfer its excitation energy to the low energy F735 chromophore, and located specifically the origin of the 730 nm fluorescence to the Lhca4 component. It was also revealed that Lhca2 and Lhca3 have identical light-harvesting properties. The isolated Photosystem I core complex showed high electron transport capacity (1535 moles O₂ mg Chl^–1 h^–1) and low fluorescence yield (0.4%) demonstrating its high functional integrity. The very rapid isolation procedure based upon perfusion chromatography should in a significant way facilitate the subfractionation of Photosystem I proteins and thereby allow more accurate functional and structural studies of individual components.Abbreviations a.u. arbitrary units - DCIP 2.6-dichlorophenol indophenol - LHC light harvesting complex     

Oxygen photoreduction and variable fluorescence during a dark-to-light transition in Chlorella pyrenoidosa

When dark-adapted (5 min in the dark) Chlorella cells were deposited on a bare platinum electrode, treated with DCMU (3-(3,4-dichlorophenyl)-1,1-dimethylurea) and illuminated, O₂ was consumed after a lag time of about 250 ms. The comparison of the O₂ consumption kinetics with the fluorescence O-I-D-P-S transition (the fast change in chlorophyll fluorescence which occurs after the onset of illumination of dark-adapted algae and is over within 2 s) observed in untreated algae indicates that no O₂ is consumed during the fluorescence rise and that O₂ uptake is initiated approximately when the maximum level of fluorescence P is reached. Mass spectrometry measurements of O₂ exchange (using ¹⁸O₂) were performed during dark to light transition with DCMU-untreated Chlorella cells. Under these conditions, O₂ reduction began after a lag time (about 200–400 ms) and stopped after about 5 s of illumination. The above experiments clearly show that the reduction of O₂ starts nearly at the same time that the fluorescence P-S decline. On the other hand, we show that the reduction of CO₂ does not interfere in the fluorescence O-I-D-P-S transient. We found the same apparent affinity for O₂ (about 57 μM) for both the fluorescence P-S decline and the reduction of O₂. At least three consecutive short (2 μs) saturating flashes were required to affect the fluorescence transient significantly and also to induce a significant uptake of O₂. Moreover, parabenzoquinone, an artificial Photosystem I electron acceptor, inhibited both the fluorescence D-P rise and the 250 ms lag time observed in the reduction of O₂. We conclude from the above results that in the early stages of the illumination of dark-adapted algae, some Photosystem I electron acceptors are in an inactive form. In this form, the electron transport chain is unable to reduce either O₂ or CO₂. This would lead to the accumulation of electrons on the Photosystem II acceptors (principally Q⁻_A and the plastoquinone pool) and therefore explains the fluorescence D-P rise. The light activation, probably achieved through the reduction of at least two electron acceptors, first allows the reduction of O₂, and therefore explains the P-S fluorescence decline. By accepting electrons before the site of regulation and mediating rapid O₂ reduction, parabenzoquinone avoids the accumulation of electrons and therefore inhibits the D-P fluorescence rise.     

Composition of the photosystems and chloroplast structure in extreme shade plants

Chloroplasts were isolated from leaves of three species of tropical rainforest plants, Alocasia macrorrhiza, Cordyline rubra and Lomandra longifolia; these species are representative of extreme “shade” plants. It was found that shade plant chloroplasts contained 4–5 times more chlorophyll than spinach chloroplasts. Their chlorophyll a/chlorophyll b ratio was 2.3 compared with 2.8 for spinach. Electron micrographs of leaf sections showed that the shade plant chloroplasts contained very large grana stacks. The total length of partitions relative to the total length of stroma lamellae was much higher in Alocasia than in spinach chloroplasts. Freeze-etching of isolated chloroplasts revealed both the small and large particles found in spinach chloroplasts.

Despite their increased chlorophyll content, low chlorophyll a/chlorophyll b ratio, and large grana, the shade plant chloroplasts were fragmented with digitonin to yield small fragments (D-144) highly enriched in Photosystem I, and large fragments (D-10) enriched in Photosystem II. The degree of fragmentation of the shade plant chloroplasts was remarkably similar to that of spinach chloroplasts, except that the subchloroplast fragments from the shade plants had lower chlorophyll a/chlorophyll b ratios than the corresponding fragments from spinach. The D-10 fragments from the shade plants had chlorophyll a/chlorophyll b ratios of 1.78-2.00 and the D-144 fragments ratios of 3.54–4.07. We conclude that Photosystems I and II of the shade plants have lower proportions of chlorophyll a to chlorophyll b than the corresponding photosystems of spinach. The lower chlorophyll a/chlorophyll b ratio of shade plant chloroplasts is not due to a significant increase in the ratio of Photosystem II to Photosystem I in these chloroplasts.

The extent of grana formation in higher plant chloroplasts appears to be related to the total chlorophyll content of the chloroplast. Grana formation may simply be an means of achieving a higher density of light-harvesting assemblies and hence a more efficient collection of light quanta.     

Excitation-energy distribution in green algae. The existence of two independent light-driven control mechanisms

Three distinct states can be identified for cells of the green alga Chlorella vulgaris; State 1 and State 2 obtained by preillumination in far-red and red light, respectively, and the dark state obtained by dark-adaptation. Addition of the inhibitor DCMU to algal cells leads to an initial rapid increase in chlorophyll-a fluorescence reflecting the closure of Photosystem II traps. This, in the case of dark and state-2-adapted algae is followed by a slow light-dependent increase to a fluorescence yield typical of State-1-adapted cells. Measurements of low temperature (77 K) emission spectra indicate that the low fluorescence yields of dark and State-2-adapted algae reflect similar balances in excitation-energy distribution between the two photosystems. In both cases, the balance favours PS I and the slow fluorescence increase seen in the poisoned algae reflects a redressing of this balance in favour of PS II. The low fluorescence yield of State-2-adapted algae is thought to be associated with the phosphorylation of chlorophyll a/b light-harvesting protein (Biochim. Biophys. Acta (1983) 724, 94–103). Measurements of the uncoupler and ATPase sensitivity of the light-dependent increases seen in DCMU-poisoned cells indicate that the low fluorescence yield of dark-adapted algae is of different origin. Evidence is presented showing that the light-driven changes in excitation-energy distribution seen in green algae involve two distinct processes; a low-intensity, wavelenght-independent change reflecting simple light/dark changes and a higher intensity, wavelength-dependent change reflecting State 1/State 2 adaptation. The former changes appear to be associated with changes in the local ionic environment within the algal chloroplast, whilst the latter appear to reflect changes in the phosphorylation state of chlorophyll a/b light-harvesting protein.     

The P700-chlorophyll a-protein of a blue-green alga

The previously isolated chlorophyll a-protein of blue-green algae has been shown to contain P700 in a ratio of 1 reaction center molecule per 100 light-harvesting chlorophyll molecules. One-fifth of the molecules in the preparation contain P700 together with some 20 light-harvesting molecules, whereas the other molecules contain bulk chlorophyll only. Both pigment-protein entities are considered to be essentially the same and cannot be fractionated. An aggregate containing both types probably makes up the photochemical portion of the algal Photosystem I in vivo. The absorption and emission spectra of the pigment-protein are reported, as well as the spectral changes associated with the photochemical reaction. In addition to chlorophyll, carotenoid and protein the complex contains a quinone, which is not a plastoquinone. This unidentified quinone appears to participate in secondary electron transfer reactions occurring in the complex. Horse cytochrome c can be bound to the complex and will donate electrons to P⁺700 upon illumination. Current hypotheses for the identity of the primary electron acceptor were tested. It appears unlikely that flavins, pteridines or iron fill this role.     

A demonstration of the physiological role of membrane phosphorylation in chloroplasts, using the bipartite and tripartite models of photosynthesis

Using the equations derived from the bipartite and tripartite models for photosynthetic organization in green plants, we have been able to characterize the effect of membrane phosphorylation on energy transduction. Phosphorylation reversibly increases (the proportion of absorbed quanta going directly to Photosystem (PS) I). This increase in we believe to be due to a decrease in the coupling between the PS II core and its associated light-harvesting complex [ΨT(3,2)·ΨT(2,3)]. Phosphorylation also reversibly increases the transfer of energy from PS II to PS I [ψT_(II→I)]. We propose that membrane phosphorylation provides the in vivo control of , ΨT(3,2)·ΨT(2,3) and ψT_(II→I). From the data we present it is clear that the changes caused in energy distribution as a result of phosphorylation are large enough to induce real changes in electron-transfer reactions. The effects of phosphorylation on these parameters are distinct from those of Mg²⁺ depletion. We have discussed changes in ΨT(3,2)·ΨT(2,3) (the coupling term) with respect to the ‘connected package’ model of photosynthetic units (Butler, W.L. (1980) Proc. Natl. Acad. Sci. U.S.A. 77, 4697–4701) and the proposed - and β-centers of PS II (Melis, A. and Homann, P.H. (1976) Photochem. Photobiol. 23, 345–350). The demonstration of changes in reversible coupling [ΨT(3,2)·ΨT(2,3)] strongly supports a connected package model in which the degree of ‘connectivity’ is under physiological control.     

Thylakoid polypeptide composition and light-independent phosphorylation of the chlorophyll a,b-protein in Prochloron, a prokaryote exhibiting oxygenic photosynthesis

Thylakoids of the prokaryote Prochloron, present as a symbiont in ascidians isolated from the Red Sea at Eilat (Israel), showed polypeptide electrophoretic patterns comparable to those of thylakoids from eukaryotic oxygen-evolving organisms. Low temperature, fluorescence spectroscopy of Prochloron, having a chlorophyll a/b ratio of 3.8–5, and frozen in situ, demonstrated the presence of Photosystem II chlorophyll-protein complex emitting at 686 and 696 nm, as well as the emission band of Photosystem I at 720 nm which was so far not observed in Prochloron species. The latter emission was absent, if the cells or thylakoids were isolated prior to freezing. Energy transfer from chlorophyll b to chlorophyll a could be demonstrated to occur in vivo. The chlorophyll a,b-protein complex of Photosystem II, isolated by non-denaturing polyacrylamide gel electrophoresis, contained one major polypeptide of 34 kDa. The polypeptide was phosphorylated in vitro by a membrane-bound protein kinase which was not stimulated by light. A light-independent protein kinase activity was also found in isolated thylakoids of another prokaryote, the cyanophyte Fremyella diplosiphon. State I–State II transition could not be demonstrated in Prochloron by measurements of modulated fluorescence intensity in situ. We suggest that the presence of a light-independent thylakoid protein kinase of Prochloron, collected in the Red Sea at not less than 30 m depth, might be the result of an evolutionary process whereby this organism has adapted to an environment in which light, absorbed preferentially by Photosystem II, prevails.     

Reactions of plastocyanin and cytochrome 553 with Photosystem I of Scenedesmus

Chloroplast material active in photosynthetic electron transport has been isolated from Scenedesmus acutus (strain 270/3a). During homogenization, part of cytochrome 553 was solubilized, and part of it remained firmly bound to the membrane. A direct correlation between membrane cytochrome 553 and electron transport rates could not be found. Sonification removes plastocyanin, but leaves bound cytochrome 553 in the membrane. Photooxidation of the latter is dependent on added plastocyanin. In contrast to higher plant chloroplasts, added soluble cytochrome 553 was photooxidized by 707 nm light without plastocyanin present. Reduced plastocyanin or cytochrome 553 stimulated electron transport by Photosystem I when supplied together or separately. These reactions and cytochrome 553 photooxidation were not sensitive to preincubation of chloroplasts with KCN, indicating that both redox proteins can donate their electrons directly to the Photosystem I reaction center. Scenedesmus cytochrome 553 was about as active as plastocyanin from the same alga, whereas the corresponding protein from the alga Bumilleriopsis was without effect on electron transport rates.

It is suggested that besides the reaction sequence cytochrome 553 → plastocyanin → Photosystem I reaction center, a second pathway cytochrome 553 → Photosystem I reaction center may operate additionally.