External electric field effects on photosynthetic membrane vesicles. Kinetic characterization of two electrophotoluminescence phases in hypotonically swollen chloroplasts

Strong externally applied electrical field pulses are known to stimulate delayed luminescence from preilluminated blebs (hypotonically swollen vesicles originating from thylakoid membranes of broken chloroplasts) by up to 3 orders of magnitude. This phenomenon is known as electrophotoluminescence. Previous analysis showed the kinetics of the electrophotoluminescence to be biphasic, displaying a rapid (R) phase which decays towards a slower one (S) (Ellenson, J.L. and Sauer, K. (1976) Photochem. Photobiol. 23, 113–123). We demonstrate that these two components represent different processes. At low pH, a good kinetic separation is obtained between the two phases, which become distinct, with the S phase manifesting also an initial rise period. Under these conditions, it is possible to estimate separately the approximate rise times of the two phases. It is shown that the R and S components have a different dependence on the pH and on the time between the actinic flash and onset of the field. The field dependence is also different, with the S phase requiring a lower threshold field than R. From these observations, it is concluded that the R and S luminescence components are formed by different precursors. The difference in behaviour of the two phases during formation of the bleb indicates that the precursors of the R and S phases belong to different parts of the bleb. We suggest that R precursors are located in the wall of the swollen thylakoid and S precursors in the membrane formations which are attached to this wall.     

Electric-field-induced luminescence emission spectra of Photosystem I and Photosystem II from chloroplasts

The electroluminescence induced by external electric fields in blebs prepared from chloroplasts consists of two kinetically different phases, rapid (R) and slow (S), which were shown to be linked to Photosystem I (PS I) and Photosystem II (PS II) activities, respectively (Symons, M., Korenstein, R. and Malkin, S. (1985) Biochim. Biophys. Acta 806, 305–310). In this report we describe conditions involving heat treatment of broken chloroplasts, which make it possible to observe R phase electroluminescence essentially devoid of any contribution by the S phase. This allowed the precise measurement of the emission spectrum of PS I electroluminescence. The emission spectrum of PS II electroluminescence was obtained using regular broken chloroplasts, which show only S-type emission. The latter emission spectrum is identical to the one obtained for ordinary prompt fluorescence, peaking at 685 nm with a bandwidth of about 25 nm. The PS I emission spectrum is symmetric around 705 nm and is much broader, about 60 nm.     

Absorbance changes due to the charge-accumulating species in System 2 of photosynthesis

Absorbance changes are reported associated with Photosystem II and showing a periodicity of two and four as a function of flash number.

The absorbance changes showing a periodicity of two were found to occur in the presence of artificial electron donors as well and are presumably caused by the secondary electron acceptor R of Photosystem II. The absorbance difference spectra suggest that R is a plastoquinone molecule, which is reduced to its semiquinone anion after an uneven number of flashes. After an even number of flashes, the semiquinone is reoxidized. The absorbance changes showing a periodicity of four are tentatively ascribed to the charge accumulating donor complex of Photosystem II.     

Energy transfer for low temperature fluorescence in PS II mutant thylakoids

The Chl-protein complexes of three maize (Zea mays L.) mutants and one barley (Hordeum vulgare L.) mutant were analyzed using low temperature Chl fluorescence emissions spectroscopy and LDS-polyacrylamide gel electrophoresis. The maize mutants hcf-3, hcf-19, and hcf-114 all exhibited a high Chl fluorescence (hcf) phenotype indicating a disruption of the energy transfer within the photosynthetic apparatus. The mutations in each of these maize mutants affects Photosystem II. The barley mutant analyzed was the well characterized Chl b-less mutant chlorina-f2, which did not exhibit the hcf phenotype. Chlorina-f2 was used because no complete Chl b-less mutant of maize is available. Analysis of hcf-3, hcf-19, and hcf-114 revealed that in the absence of CP43, LHC II can still transfer excitation energy to CP47. These results suggest that in mutant membranes LHC II can interact with CP47 as well as CP43. This functional interaction of LHC II with CP47 may only occur in the absence of CP43, however, it is possible that LHC II is positioned in the thylakoid membranes in a manner which allows association with both CP43 and CP47.Abbreviations hcf high chlorophyll fluorescence - LDS lithium dodecyl sulfate - LHC II light-harvesting complex of Photosystem II - LHC I light-harvesting complex of Photosystem I - CPIa chlorophyll-protein complex consisting of LHC I and the PS I core complex - CPI chlorophyll-protein complex consisting of the PS I core complex - CP47 47 kDa chlorophyll-protein of the Photosystem II core - CP43 43 kDa chlorophyll-protein of the Photosystem II core - CP29 29 kDa chlorophyll-protein of Photosystem II - CP26 26 kDa chlorophyll-protein of Photosystem II - CP24 24 kDa chlorophyll-protein of Photosystem II - fp free pigments     

A quantitative study of the slow decline of chlorophyll a fluorescence in isolated chloroplasts.

A detailed study of the photo-induced decline in chlorophyll a fluorescence intensity (Kautsky phenomenon) in coupled isolated chloroplasts from a high level (P) to a low stationary level (S) is presented. 1. A linear relationship between P leads to S quenching and intrathylakoid H+ concentration was found. When the light-induced proton gradient was abolished by uncoupling, the fluorescence emission at room temperature was lowered proportionally to increased H+ concentration in the medium. 2. Fluorescence spectra at -196 degrees C of samples frozen at the P and S states showed no significant differences in the Photosystem I/Photosystem II ratio of fluorescence emission. Furthermore, freezing to -196 degrees C reversed the P leads to S quenching. This indicates that the P leads to S quenching is not related to an increase of spillover of excitation energy from Photosystem II to Photosystem I. 3. When Mg2+ was added to thylakoids suspended in a medium free of divalent cations, the inhibition of spillover required lower Mg2+ concentrations (half saturation at 0.6 mM). Increased proton concentration in the medium also inhibited spillover. 4. The results are interpreted in terms of two sites of Mg2+ and H+ effects on excitation deactivation in Photosystem II. One site is located on the outer face of the thylakoid membrane; action of both Mg2+ and H+ at this side diminishes spillover. The second site is located on the inner face of the membrane; as Mg2+ is displaced there by protons, a non-photochemical quenching of Photosystem II fluorescence is induced, which is manifested by the P leads to S decline.     

Spectral and kinetic analysis of the energy coupling in the PS I-LHC I supercomplex from the green alga Chlamydomonas reinhardtii at 77 K

Energy transfer processes in the chlorophyll antenna of the PS I-LHCI supercomplexes from the green alga Chlamydomonas reinhardtii have been studied at 77 K using transient absorption spectroscopy with multicolor excitation in the 640-670 nm region. Comparison of the kinetic data obtained at low and room temperatures indicates that the slow approximately approximately 100 ps excitation equilibration phase that is characteristic of energy coupling of the LHCI peripheral antenna to the PS I core at physiological temperatures (Melkozernov AN, Kargul J, Lin S, Barber J and Blankenship RE (2004) J Phys Chem B 108: 10547-10555) is not observed in the excitation dynamics of the PS I-LHCI supercomplex at 77 K. This suggests that at low temperatures the peripheral antenna is energetically uncoupled from the PS I core antenna. Under these conditions the observed kinetic phases on the time scales from subpicoseconds to tens of picoseconds represent the superposition of the processes occurring independently in the PS I core antenna and the Chl a/b containing LHCI antenna. In the PS I-LHCI supercomplex with two uncoupled antennas the excitation is channeled to the excitation sinks formed at low temperature by clusters of red pigments. A better spectral resolution of the transient absorption spectra at 77 K results in detection of two DeltaA bands originating from the rise of photobleaching on the picosecond time scale of two clearly distinguished pools of low energy absorbing Chls in the PS I-LHCI supercomplex. The first pool of low energy pigments absorbing at 687 nm is likely to originate from the red pigments in the LHCI where the Lhca1 protein is most abundant. The second pool at 697 nm is suggested to result either from the structural interaction of the LHCI and the PS I core or from other Lhca proteins in the antenna. The kinetic data are discussed based on recent structural models of the PS I-LHCI. It is proposed that the uncoupling of pigment pools may be a control mechanism that regulates energy flow in Photosystem I.     

Identification of polypeptides of photosystem I reaction center as the products of chloroplast genes PS1A1 and PS1A2

The Photosystem I Reaction Center of spinach was found to contain two polypeptides of approximate apparent Mr of 56,000 and 64,000. the 56 kDa polypeptide was identified as the product of chloroplast gene PS1A1 using an antibody specific for the PS1A1 gene product of corn. Presumably the 64 kDa polypeptide is the product of gene PS1A2.     

Properties of ATP-induced chlorophyll luminescence in chloroplasts.

1. The recently described reaction of ATP-induced luminescence is analyzed for its relation to other ATP-induced reactions such as ATP-driven transmembrane proton gradient formation and ATP-driven reverse electron flow. 2. In the absence of phenazine methosulfate ATP-induced luminescence is optimal while the main phase of ATP-driven reverse electron flow is eliminated. 3. DCMU which by itself causes a much smaller luminescence, inhibits the ATP-induced luminescence. 4. Nigericin plus valinomycin, but not each by itself, fully inhibit the ATP-induced luminescence. 5. The observations are interpreted as indicating that ATP stimulates luminescence by a 2-fold mechanism: (a) increasing the amount of the reducing primary electron acceptor of Photosystem II, Q, and (b) creating a transmembrane electrochemical potential which serves to decrease the activation energy required for the charge recombination reaction which leads to luminescence.     

Relation between slow delayed light emission and acid-base triggered luminescence in chloroplasts

Acid-base triggered luminescence in relation to slow delayed light emission (> 3 s) was studied in chloroplasts. After analyzing their time courses, the acid-base induced luminescence curve was found to return to the original curve of delayed light emission. Peaks of the acid-base triggered luminescence induced after various darkness periods following preillumination decreased parallel to the time course of delayed light emission without base treatment. 3-(3,4-Dichlorophenyl)-1,1-dimethylurea enhanced both the delayed light emission and acid-base induced luminescence, while carbonyl cyanide m-chlorophenylhydrazone inhibited both. Several photophosphorylation uncouplers inhibited the acid-base induced luminescence without any substantial effect on the delayed light emission. It is concluded that the acid-base triggered luminescence is not caused by the reversion of electrons from remote intermediates on the reducing side of Photosystem II. The possibility of the presence of an activation pathway for the acid-base triggered luminescence which differs from that of the delayed light emission is also discussed.     

The sensitivity of Photosystem II to damage by UV-B radiation depends on the oxidation state of the water-splitting complex

The water-oxidizing complex of Photosystem II is an important target of ultraviolet-B (280-320 nm) radiation, but the mechanistic background of the UV-B induced damage is not well understood. Here we studied the UV-B sensitivity of Photosystem II in different oxidation states, called S-states of the water-oxidizing complex. Photosystem II centers of isolated spinach thylakoids were synchronized to different distributions of the S(0), S(1), S(2) and S(3) states by using packages of visible light flashes and were exposed to UV-B flashes from an excimer laser (lambda=308 nm). The loss of oxygen evolving activity showed that the extent of UV-B damage is S-state-dependent. Analysis of the data obtained from different synchronizing flash protocols indicated that the UV-sensitivity of Photosystem II is significantly higher in the S(3) and S(2) states than in the S(1) and S(0) states. The data are discussed in terms of a model where UV-B-induced inhibition of water oxidation is caused either by direct absorption within the catalytic manganese cluster or by damaging intermediates of the water oxidation process.     

Photoreduction of pheophytin in reaction centers of the photosystem II in intact cells of green algae and cyanobacteria under anaerobic conditions

Reversible photoreduction of pheophytin (Pheo) accompanied by a decrease in the chlorophyll fluorescence yield is observed in Photosystem 2 of the intact cells of green algae and cyanobacteria under anaerobic conditions. The photoreaction is inhibited by DCMU and reactivated upon subsequent addition of either ascorbate of dithionite. It is suggested that as a result of electron donation from the water splitting system being in the state S(3), to the reaction centre of Photosystem 2 in the state [P(+)(680)Pheo(-)] Q(-) after the primary photoreaction there occurs formation of the long-living state [P(680)Pheo(-)] Q(-). It was found that oxidized NADP, benzyl viologen and methyl viologen accelerate oxidation of Pheo reduced int he Photosystem 2 in the light indicating that these electron acceptors (typical for Photosystem 1) can accept an election from Pheo in Photosystem 2.     

Expression of ELIPs and PS II-S protein in spinach during acclimative reduction of the Photosystem II antenna in response to increased light intensities

The PS II-S protein and the so-called early light-inducible proteins (ELIPs) are homologous to the chlorophyll a/b-binding (Cab) gene products functioning in light-harvesting. The functional significance of these two CAB homologues is not known although they have been considered to bind pigments and in the case of the PS II–S protein this has been experimentally supported. The role of these two proteins does not appear to be light-harvesting but instead they are suggested to play a role as quenchers of free chlorophyll molecules during biogenesis and/or degradation of pigment-binding proteins. Such a role would be essential to eliminate the toxic and damaging effects that can be induced by free chlorophyll in the light. To this end the expression and characteristics of the ELIPs and the PS II–S protein were investigated in spinach leaves acclimating from low to high light intensities. Under these conditions there is a reduction in the antenna size of Photosystem II due to proteolytic digestion of its major chlorophyll a/b-binding protein (LHC II). During this acclimative proteolysis, up to one third of LHC II can be degraded and consequently substantial amounts of chlorophyll molecules will lose their binding sites. Our results reveal that there is a close correlation between ELIP accumulation and the onset of the LHC II degradation as low light-grown spinach leaves are subjected to increased light intensities. In contrast, there was no change in the relative level of the PS II–S protein during the acclimation process. It is concluded that the role for the ELIPs may be related to binding of liberated chlorophyll molecules and quenching of the toxic effects during LHC II degradation. In addition it was shown that in spinach four different ELIP species can be expressed and that they show different accumulation patterns in response to increased light intensities.     

Evidence for a close spatial location of the binding sites for CO2 and for photosystem II inhibitors

1. CO2-depletion of thylakoid membranes results in a decrease of binding affinity of the Photosystem II (PS II) inhibitor atrazine. The inhibitory efficiency of atrazine, expressed as I50-concentration (50% inhibition) of 2,6-dichlorophenolindophenol reduction, is the same in CO2-depleted as well as in control thylakoids. This shows that CO2-depletion results in a complete inactivation of a part of the total number of electron transport chains. 2. A major site of action of CO2, which had previously been located between the two electron acceptor quinone molecule B (or R) and Photosystem II inhibitor atrazine as suggested by the following observations: (a) CO2-depletion results in a shift of the binding constant (kappa b) of [14C]atrazine to thylakoid membranes indicating a decreased affinity of atrazine to membrane; (b) trypsin treatment, which is known to modify the Photosystem II complex at the level of B, strongly diminishes CO2 stimulation of electron transport reactions in CO2-depleted membranes; and (c) thylakoids from atrazine-resistant plants, which contain a Photosystem II complex modified at the inhibitor binding site, show an altered CO2-stimulation of electron flow. 3. CO2-depletion does not produce structural changes in enzyme complexes involved in Photosystem II function of thylakoid membranes, as shown by freeze-fracture studies using electron microscopy.     

Comparative studies on the polypeptide composition of chloroplast lamellae and lamellar fractions

The polypeptide composition of spinach chloroplast membranes and membrane fractions has been examined by the technique of sodium dodecylsulfate-polyacrylamide gel electrophoresis. Chloroplasts were fragmented into grana (Photosystem II enriched) and stroma lamellae (Photosystem I in character) by the French press technique. The grana lamellae were futher fractionated by the use of digitonin into two fractions, one enriched in Photosystem II and the other enriched in Photosystem I. These membranes are composed of at least 15 polypeptides two of which, with approximate weights of 39 and 50 kdaltons, are observed only in granal fractions. Quantitatively the primarily Photosystem II fractions are enriched in polypeptides in the 30-23 kdalton range whereas the Photosystem I (or Photosystem I-enriched) fractions are enriched in polypeptides in the 60-54 kdalton region. The experiments reported show that contamination by soluble proteins or other membranes is negligible. The results indicate that subtle differences in composition account for the large differences in structure and function within the chloroplast membrane system.     

Light-induced FTIR difference spectroscopy of the S(2)-to-S(3) state transition of the oxygen-evolving complex in Photosystem II

We have applied flash-induced FTIR spectroscopy to study structural changes upon the S(2)-to-S(3) state transition of the oxygen-evolving complex (OEC) in Photosystem II (PSII). We found that several modes in the difference IR spectrum are associated with bond rearrangements induced by the second laser flash. Most of these IR modes are absent in spectra of S(2)/S(1), of the acceptor-side non-heme ion, of Yradical(D)/Y(D) and of S(3)'/S(2)' from Ca-depleted PSII preparations. Our results suggest that these IR modes most likely originate from structural changes in the oxygen-evolving complex itself upon the S(2)-to-S(3) state transition in PSII.     

Dark reduction of QA in intact barley leaves as an effect of lowered CO2 concentration monitored by chlorophyll a luminescence and chlorophyll a F0 dark fluorescence

When the CO₂ concentration in the atmosphere above an intact barley leaf was lowered in the dark after illumination, chlorophyll a luminescence and chlorophyll a dark fluorescence were stimulated. The stimulation was induced by lowered levels of CO₂ in a wide concentration range including concentrations well above that saturating photosynthesis. The stimulation of luminescence by lowered CO₂ concentrations was more pronounced after far-red excitation than after white light excitation. The difference in response to lowered CO₂ concentrations after white/far-red excitation was less pronounced for fluorescence than for luminescence. Stimulation of luminescence was more pronounced when the CO₂ concentration was lowered in an O₂-containing atmosphere than under anaerobic conditions. It is concluded that lowering of the CO₂ concentration in the dark after illumination causes a partial reduction of the primary Photosystem II acceptor Q_A.     

Effect of complete extraction and re-addition of manganese on thermoluminescence of pea Photosystem II preparations

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

Graphical and numerical analysis of thermoluminescence and fluorescence F0 emission in photosynthetic material

A set-up for recording thermoluminescence emission together with the constant F₀ fluorescence yield is described briefly. It is driven by a microcomputer through plugged-in cards.Practical aspects of the simulation of TL bands and of decomposition of complex TL signals are examined. A reproducible and linear temperature gradient and the use of photon counting for luminescence detection are important features for further analyzing the recorded signal. The simulation procedure used is a step-by-step calculation of the number of charge recombinations, which is then substracted from the number of remaining charge pairs able to produce luminescence. This procedure consists first of a graphical fitting, followed by a numerical minimization, with a maximum of five simulated components. The quality of the simulation is evaluated by the sum of squares of differences (signal-simulation), related to the signal area. Equivalent decomposition patterns may be found for the same recording and additional information is needed for interpretation of TL data. Averaging signals is feasible, provided that maximum temperatures Tm of averaged bands are sufficiently similar (±3°C). Simultaneous measurement of the antenna fluorescence yield F₀, using an ultra-weak pulsed blue LED, gives an estimate of the luminescence yield. This has to be taken into account in the analysis of the Q band and of high temperature (>40°C) bands.The simulation parameters appear to be dependent on plant growth conditions. Quantitative analysis of thermoluminescence emission could be useful in the study of the effects of climatic factors on the photosynthetic apparatus in plants.Abbreviations PS-II Photosystem II - TL thermoluminescence - F₀ constant fluorescence emission, under ultra-low light intensity - Q_A and Q_B respectively, primary and secondary electron acceptors of Photosystem II - S₂ and S₃ respectively, the two and three positively charged states of the oxygen evolving system - SSD sum of squares of differences between the signal and a simulation (fitting) or between the signal and a smoothed curve (noise)     

Evidence for the existence of [2Fe-2S] as well as [4Fe-4S] clusters among FA,FB and FX. Implications for the structure of the Photosystem I reaction center

Core extrusion of the bound iron-sulfur centers from spinach Photosystem I showed the presence of [2Fe-2S] clusters as well as [4Fe-4S] clusters among F_A, F_B and F_X. Extrusion of the iron-sulfur ensemble was not quantitative; however, the presence of [2Fe-2S] clusters correlated with higher concentration of unfolding solvent. Since F_X is highly resistant to denaturation, and since F_A and F_B are known to contain [4Fe-4S] clusters, the [2Fe-2S] clusters are assigned to F_X. The presence of [2Fe-2S] clusters in Photosystem I has significance in the structure and organization of F_X on the reaction center. Since four cysteinyl ligands are assumed to hold an iron-sulfur cluster, a Photosystem I subunit may consist of two approx. 64-kDa proteins bridged by a single [2Fe-2S] cluster. The complete reaction center would consist of two subunits positioned so that two [2Fe-2S] clusters are in magnetic interaction, thereby constituting F_X.     

Isolation and characterization of photosystem I and II membrane particles from the blue-green alga, Synechococcus cedrorum.

Fractions enriched in either Photosystem I or Photosystem II activity have been isolated from the blue-green alga, Synechococcus cedrorum after digitonin treatment. Sedimentation of this homogenate on a 10--30% sucrose gradient yielded three green bands: the upper band was enriched in Photosystem II, the lowest band was enriched in Photosystem I, while the middle band contained both activities. Large quantities of both particles were isolated by zonal centrifugation, and the material was then further purified by chromatography on DEAE-cellulose. The resulting Photosystem II particles carried out light-induced electron transport from semicarbizide to ferricyanide of over 2000 mumol/mg Chlorophyll per h (which was sensitive to 3-(3,4-dichlorophenyl)-1, 1-dimethylurea), and was nearly devoid of Photosystem I activity. This particle contains beta-carotene, very little phycocyanin, has a chlorophyll absorption maximum at 675 nm, and a liquid N2 fluorescence maximum at 685 nm. The purest Photosystem II particles have a chlorophyll to cytochrome b-559 ratio of 50 : 1. The Photosystem I particle is highly enriched in P-700, with a chlorophyll to P-700 ratio of 40 : 1. The physical structure of the two Photosystem particles has also been studied by gel electrophoresis and electron microscopy. These results indicate that the size and protein composition of the two particles are distinctly different.