ATP-induced quenching of chlorophyll fluorescence in chloroplasts of higher plants. Dependence on structural properties of the membranes

The ATP-induced quenching of chlorophyll fluorescence in chloroplasts of higher plants is shown to be inhibited when the mobility of the protein complexes into the thylakoid membranes is reduced. Its occurrence also requires the presence of LHC complexes and the ability of the membranes to unstack. These observations, in addition to a slight increase of charge density of the surface—as indicated by 9-aminoacridine fluorescence and high salt-induced chlorophyll fluorescence studies—and partial unstacking of the membranes—as monitored by digitonin method and 540 nm light scattering changes—after phosphorylation, suggest that the ATP-induced quenching of chlorophyll fluorescence could reflect some lateral redistribution of membrane proteins in the lipid matrix of the thylakoids.     

Characterisation of the effects of Antimycin A upon high energy state quenching of chlorophyll fluorescence (qE) in spinach and pea chloroplasts

High energy state quenching of chlorophyll fluorescence (qE) is inhibited by low concentrations of the inhibitor antimycin A in intact and osmotically shocked chloroplasts isolated from spinach and pea plants. This inhibition is independent of any effect upon pH (as measured by 9-aminoacridine fluorescence quenching). A dual control of qE formation, by pH and the redox state of an unidentified chloroplast component, is implied. Results are discussed in terms of a role for qE in the dissipation of excess excitation energy within photosystem II.Abbreviations 9-AA_max = Maximum yield of 9-aminoacridine fluorescence - DCMU = 3(3,4-dichlorophenyl)-1,1-dimethylurea; F_max ± Maximum yield of chlorophyll fluorescence - hr = hour - PAR = Photosynthetically Active Radiation - Q_A = Primary stable electron acceptor within photosystem II - qE = High energy state quenching of chlorophyll fluorescence - qI = quenching of chlorophyll fluorescence related to photoinhibition - qP = Quenching of chlorophyll fluorescence by oxidised plastoquinone - qQ = photochemical quenching of chlorophyll fluorescence - qR = (F_max—maximum level of chlorophyll fluorescence induced by the addition of saturating DCMU) - qT = Quenching of chlorophyll fluorescence attributable to state transitions     

The cation-dependence of the degree of protein phosphorylation-induced unstacking of pea thylakoids

Experiments are presented to show that the phosphorylation of the light-harvesting chlorophyll $\text{a}\text{b}\text{-}\text{protein}$ complex (LHC) induces structural reorganisation within the thylakoid membrane in response to the introduction of additional negative surface charges. The effect of cations of different valency on chlorophyll fluorescence measurements indicates that LHC-phosphorylation-induced reorganisation involves a change in the electrostatic screening capability of the added cation. At intermediate levels of cations (e.g., 1 or 2 mM Mg²⁺), which substantially stack non-phosphorylated membranes, it was found that membrane phosphorylation caused considerable unstacking as monitored by light scattering and electron microscopy. Concomitant with this was a large decrease in chlorophyll fluorescence indicative of randomisation of chlorophyll protein complexes which would result in an increase in energy transfer between the photosystems as well as an absorption cross-section change. At higher concentrations (e.g., above 5 mM Mg²⁺) a persistent ATP-induced decrease in chlorophyll fluorescence has been attributed to the displacement of charged phosphorylated LHC from the appressed granal to the non-appressed stromal lamellae, thus decreasing the absorption cross-section of Photosystem II. Under these circumstances only a small degree of unstacking was detected by light scattering and measurements of the percentage of thylakoid length which is stacked to form grana. However, when considered on a surface area basis, the structural changes observed can qualitatively account for the magnitude of the chlorophyll fluorescence quenching due to the lateral diffusion of LHC.     

Photosynthetic control, “energy-dependent” quenching of chlorophyll fluorescence and photophosphorylation under influence of tertiary amines

The effects of the tertiary amines tetracaine, brucine and dibucaine on photophosphorylation and control of photosynthetic electron transport in isolated chloroplasts of Spinacia oleracea were investigated. Tertiary amines inhibited photophosphorylation while the related electron transport decreased to the rates, observed under non-phosphorylating conditions. Light induced quenching of 9-aminoacridine fluorescence and uptake of ¹⁴C-labelled methylamine in the thylakoid lumen declined in parallel with photophosphorylation, indicating a decline of the transthylakoid proton gradient. In the presence of ionophoric uncouplers such as nigericin, no effect of tertiary amines on electron transport was seen in a range of concentration where photophosphorylation was inhibited. Under the influence of the tertiary amines tested, pH-dependent feed-back control of photosystem II, as indicated by energy-dependent quenching of chlorophyll fluorescence, was unaffected or even increased in a range of concentration where 9-aminoacridine fluorescence quenching and photophosphorylation were inhibited. The data are discussed with respect to a possible involvement of localized proton flow pathways in energy coupling and feed-back control of electron transport.Abbreviations 9-AA 9-aminoacridine - J _e flux of photosynthetic electron transport - PC photosynthetic control - pH₁ H⁺ concentration in the thylakoid lumen - pmf proton motive force - _P potential quantum yield of photochemistry of photosystem II (with open reaction centers) - Q _A primary quinone-type electron acceptor of photosystem II - q _Q photochemical quenching of chlorophyll fluorescence - q _E energy-dependent quenching of chlorophyll fluorescence - q _AA light-induced quenching of 9-amino-acridine fluorescence     

The fluorescent properties of acridines in the presence of chloroplasts or liposomes. On the quantitative relationship between the fluorescence quenching and the transmembrane proton gradient

The fluorescent properties of 9-aminoacridine were studied in chloroplasts and phospholipid liposomes.

In energized chloroplasts it was found that the percentage of fluorescence quenching was dependent on both the 9-aminoacridine concentration and the chlorophyll concentration. On the other hand, it was independent of the osmolarity of the medium.

In phospholipid liposomes the dependence of the fluorescence quenching on the concentration of 9-aminoacridine was similar to that in chloroplasts. Moreover, the fluorescence quenching depended on the presence of charged compounds in the membrane being larger in negatively charged than in positively charged liposomes.

The fluorescence of both the monoamine 9-amino-6-chloro-2-methoxyacridine and the diamine atebrin is quenched more extensively than that of 9-aminoacridine. Although the percentage of fluorescence quenching of both atebrin and 9-aminoacridine is dependent on the outside pH, the relationship between the fluorescence quenching of the two probes under similar conditions is not pH-dependent.

It is concluded that calculation of ΔpH from the percentage of fluorescence quenching of fluorescent amines is not meaningful, that the osmotic volume of chloroplasts is not involved in the quenching process and, consequently, that the interaction between the acridines and energized membranes is more likely to occur at the level of the membrane proper.     

Consequences of LHC II deficiency for photosynthetic regulation in chlorina mutants of barley

The light-harvesting chlorophyll a/b proteins associated with PS II (LHC II) are often considered to have a regulatory role in photosynthesis. The photosynthetic responses of four chlorina mutants of barley, which are deficient in LHC II to varying degrees, are examined to evaluate whether LHC II plays a regulatory role in photosynthesis. The efficiencies of light use for PS I and PS II photochemistry and for CO₂ assimilation in leaves of the mutants were monitored simultaneously over a wide range of photon flux densities of white light in the presence and absence of supplementary red light. It is demonstrated that the depletions of LHC II in these mutants results in a severe imbalance in the relative rates of excitation of PS I and PS II in favour of PS I, which cannot be alleviated by preferential excitation of PS II. Analyses of xanthophyll cycle pigments and fluorescence quenching in leaves of the mutants indicated that the major LHC II components are not required to facilitate the light-induced quenching associated with zeaxanthin formation. It is concluded that LHC II is important to balance the distribution of excitation energy between PS I and PS II populations over a wide range of photon flux densities. It appears that LHC II may also be important in determining the quantum efficiency of PS II photochemistry by reducing the rate of quenching of excitation energy in the PS II primary antennae.Abbreviations Fm, Fv maximal and variable fluorescence yields in a light adapted state - LHC II light harvesting chlorophyll a/b protein complex associated with PS II - q_p photochemical quenching - A₈₂₀ light-induced absorbance change at 820 nm - ø_PSI, ø_PSII relative quantum efficiencies of PS I and PS II photochemistry - øCO₂ quantum yield of CO₂ assimilation     

The quenching characteristics of potassium iridic chloride and their meaning for the origin of chlorophyll fluorescence components

To understand the origins of the different lifetime components of photosystem 2 (PS2) chlorophyll (Chl) fluorescence we have studied their susceptibility to potassium iridic chloride (K₂IrCl₆) which has been shown to bleach antenna pigments of photosynthetic bacteria (Loach et al. 1963). The addition of K₂IrCl₆ to PS2 particles gives rise to a preferential quenching of the variable Chl fluorescence (F_v). At concentrations lower than 20 M, this is brought about mainly by a decrease in the yield, but not in the lifetime, of the slowest component when all the PS2 reaction centres are closed (F_M). The yield of the middle and fast decays are not significantly altered. This type of quenching is not seen with DNB. The iridate-induced quenching of the initial fluorescence level (F₀) is due to a proportional decrease in the yield and lifetime of the three components and correlates with the observed modification in the relative quantum yield of oxygen evolution. In this concentration range a bleaching of Chl a is seen. At higher iridate levels, greater than 20 M, a proportional decrease in the lifetimes and yields of the three kinetic components is seen at F_M. These changes are associated with a carotenoid bleaching. In isolated light harvesting Chl a/b complexes of PS2 (LHC2), iridate addition converts a 4 ns decay into a 200 ps emission and both types of bleaching are observed. By also measuring the rate of PS2 trap closure versus iridate concentration, we have discussed the results in terms of excitation energy transfer.Abbreviations DNB m-dinitrobenzene - F_M maximum Chl fluorescence - F₀ initial fluorescence - F_v variable fluorescence - I pheophytin a primary electron acceptor of PS2 - P₆₈₀ chlorophyll a of photochemical centre - PS2 photosystem 2 - Q_A primary stable electron acceptor of PS2 - Chl chlorophyll - LHC2 light harvesting Chl a/b complex of PS2 - MES 2(N-morpholino) ethanesulfonic acid - DCMU 3-(3-4-dichlorophenyl) 1-1 dimethylurea - PPBQ phenyl-p-benzo-quinone - BBY PS2-enriched membranes prepared as in Berthold et al. (1981) - Q₄₀₀ PS2 electron acceptor with a midpoint potential of 400 mV     

9-Aminoacridine as a fluorescent probe of the electrical diffuse layer associated with the membranes of plant mitochondria.

1. Mitochondria from Jerusalem artichoke (Helianthus tuberosus) tubers and Arum maculatum spadices caused a quenching of the fluorescence of 9-aminoacridine when mixed in a low-cation medium (approximately 1 mM-K+) and addition of chelators further decreased the fluorescence. Salts released the quenching of the 9-aminoacridine fluorescence and the efficiency of the release appeared to be mainly dependent on the valency of the cation (C3+ greater than C2+ greater than C+). 2. The results are consistent with the theory of charge screening and demonstrate that 9-aminoacridine is a convenient probe of the behaviour of cations on the membranes of mitochondria and in the diffuse layer associated with these membranes. 3. The concentration of salt required to achieve half-maximal release of quenching of 9-aminoacridine fluorescence was proportional to the concentration of mitochondria in the solution and theoretical considerations show this effect to be inherent in the Gouy-Chapman theory. 4. 9-Aminoacridine was removed from the bulk of the solution by the mitochondria to a far greater extent than was Na+ or K+, which is suggested to be due to the formation of bi- and poly-valent cations by aggregation of 9-aminoacridine molecules in the diffuse layer. This would have implications for the use of 9-aminoacridine to determine delta pH across membranes. 5. Jerusalem-artichoke mitochondria removed from 9-aminoacridine and Ca2+ from the bulk of the solution and required more ions to screen the membranes than did an equal concentration (mg of protein/ml) of Arum mitochondria, indicating that Jerusalem-artichoke mitochondria contain more negative charges per mg of protein.     

The effect of high-energy-state excitation quenching on maximum and dark level chlorophyll fluorescence yield

The quenching of variable fluorescence yield (q_N) and the quenching of dark level fluorescence yield (q₀) directly atributable to high-energy-state fluorescence quenching (q_E) was studied to distinguish between energy dissipation in the antenna and light harvesting complexes (antenna quenching) and energy dissipation at the reaction centres (reaction centre quenching). A consistent relationship was obtained between q_N and q₀ in barley leaves, the green alga Dunaliella C9AA and in pea thylakoids with 2,3,5,6-tetramethyl-p-phenylene diamine (DAD) as mediator of cyclic electron flow around PS 1. This correlated well with the relationship obtained using m-dinitrobenzene (DNB), a chemical model for antenna quenching, to quench fluorescence in Dunaliella C9AA or pea thylakoids. The results also correlated reasonably well with theoretical predictions by the Butler model for antenna quenching, but did not correlate with the predictions for reaction centre quenching. It is postulated that q_E quenching therefore occures in the antenna and light harvesting complexes, and that the small deviation from the Butler prediction is due to PS 2 heterogeneity.Abbreviations 9-aa 9-aminoacridine - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - EDTA Ethylenediaminetetra-acetic acid - Hepes 4-(2-hydroxyethyl)-1-piperazineethanesulphonic acid - Mes 2-(N-morpholino) prophanesulfonate - PS 1 photosystem 1 - PS 2 photosystem 2 - Q_A and Q_B primary and secondary stable electron acceptors of photosystem 2 - q_N non-photochemical fluorescence quenching coefficient - q_E high-energy-state fluorescence quenching coefficient - q₀ quenching coefficient for F₀ - F₀ dark level fluorescence yield - F_m maximum fluorescence yield - F_v variable fluorescence yield - F_v/F_m ratio of variable to total fluorescence yield - DAD 2,3,5,6-tetramethyl-p-phenylene diamine - DNB m-dinitrobenzene     

Complex formation in plant thylakoid membranes. Competition studies on membrane protein interactions using synthetic peptide fragments

Thylakoid membranes of pea were used to study competition between extra-membrane fragments and their parental membrane-bound proteins. Phosphorylated and unphosphorylated fragments of light harvesting complex II (LHC II) from higher plants were used to compete with LHC II for interactions with itself and with other thylakoid protein complexes. Effects of these peptide fragments of LHC II and of control peptides were followed by 80 K chlorophyll fluorescence spectroscopy of isolated thylakoids. The phosphorylated LHC II fragment competes with membrane-bound phosphoproteins in the phosphatase reaction. The same fragment accelerates the process of dark-to-light adaptation and decreases the rate of the light-to-dark adaptation when these are followed by fluorescence spectroscopy. In contrast, the non-phosphorylated LHC II peptide does not affect the rate of adaptation but produces results consistent with inhibition of formation of a quenching complex. In this quenching complex we propose that LHC II remains inaccessible to the LHC II kinase, explaining an observed decrease in LHC II phosphorylation in the later stages of the time-course of phosphorylation. The most conspicuous protein which is steadily phosphorylated during the time-course of phosphorylation is the 9 kDa (psbH) protein. The participation of the phosphorylated form of psbH in the quenching complex, where it is inaccessible to the phosphatase, may explain its anomalously slow dephosphorylation. The significance of the proposed complex of LHC II with phospho-psbH is discussed.Abbreviations LHC II light harvesting complex II - PS II Photosystem II - PS I Photosystem I     

Phospholipase A2 induced effects on the structural organization and physical properties of pea chloroplast membranes

Phospholipase A₂ (PLA₂)-induced effects on the membrane organization, fluidity properties and surface charge density of pea chloroplasts were investigated. It was observed that lipolytic treatment with PLA₂ altered the chloroplast structure having as a result a swelling of thylakoids and a total destruction of normal granal structure. In spite of this, the thylakoid membranes remained in close contact. At the same time, a slight decrease of surface charge density was registered, thus explaining the adhesion of swelled membranes. Fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene (DPH) was measured during PLA₂ treatment. A pronounced decrease of DPH fluorescence polarization was found, indicating that phospholipase treatment resulted in considerable disordering and/or fluidization of the thylakoid membranes. The increased fluidity could be attributed to the destabilizing effect of the products of enzymatic hydrolysis of the phospholipids (free fatty acids, lysophospholipids) on the bilayer structure of thylakoids membranes.Abbreviations 9-AA 9-aminoacridine - BSA bovine serium albumin - DCMU 3-/3,4-dichlorophenyl-1,1-dimethyl/urea - DPH 1,6-diphenyl-1,3,5-hexatriene - EDTA ethylenediaminetetraacetic acid - HEPES N-2-hydroxyethylpiperazine-N-2-ethanesulfonic acid - LHC light harvesting chlorophyll a/b-protein complex of PS II - MES 2/N-morpholine/ethanesulfonic acid - PLA₂ phospholipase A₂ - PS I, PS II photosystem I and photosystem II, respectively - S lipid structural order parameter - THF tetrahydrofuran - TRICINE N-/tris/hydroxymethyl/methyl/glicine     

An active Mehler-peroxidase reaction sequence can prevent cyclic PS I electron transport in the presence of dioxygen in intact spinach chloroplasts

Simultaneous measurements of 9-aminoacridine (9-AA) fluorescence quenching, O₂-uptake and chlorophyll fluorescence of intact spinach chloroplasts were carried out to assess the relationship between the transthylakoidal pH and linear electron flux passing through Photosystem II. Three different types of O₂-dependent electron flow were investigated: (1) Catalysed by methyl viologen; (2) in the absence of a catalyst and presence of an active ascorbate peroxidase (Mehler-peroxidase reaction); (3) in the absence of a catalyst and with the ascorbate peroxidase being inhibited by KCN (Mehler reaction). The aim of this study was to assess the relative contribution of pH-formation which is not associated with electron flow through Photosystem II and, which should reflect Photosystem I cyclic flow under the different conditions. The relationship between the extent of 9-AA fluorescence quenching and O₂-uptake rate was found to be almost linear when methyl viologen was present. In the absence of methyl viologen (Mehler reaction) an increase of 9-AA fluorescence quenching to a value of 20% at low light intensities was associated with considerably less O₂-uptake than in the presence of methyl viologen, indicating the involvement of cyclic flow. These findings are in agreement with a preceding study of Kobayashi and Heber (1994). However, when no KCN was added, such that the complete Mehler-peroxidase reaction sequence was operative, the relationship between 9-AA fluorescence quenching and the flux through PS II, as measured via the chlorophyll fluorescence parameter F/Fm × PAR, was identical to that observed in the presence of methyl viologen. Under the assumption that methyl viologen prevents cyclic flow, it is concluded that there is no significant contribution of cyclic electron flow to pH-generation in intact spinach chloroplasts.     

A comparative analysis of the effects of in-vivo and in-vitro abscisic-acid treatment on the surface electrical properties of barley chloroplast membranes

The effects of in-vivo and in-vitro abscisic acid (ABA) treatments on the surface charge density () of barley (Hordeum vulgare L.) thylakoids were compared using 9-aminoacridine fluorescence. The estimated surface charge density of isolated thylakoid membranes from control (non-treated) barley leaves was-0.065 C · m^-2. The net negative surface charge density decreased after application of various concentrations of ABA (10^-6, 10^-5 M) for 7 d in-vivo, the more pronounced effect being observed at 10^-5 M ABA. When ABA was added to the suspension of isolated thylakoids the opposite effect was observed. The average charge density increased in in-vitro-treated thylakoids at 10^-5 M ABA to -0.081 C · m^-2. The results are discussed in terms of a specific ABA-induced influence of the composition and-or stoicheometry of charged protein complexes within the thylakoid membranes.Abbreviations and Symbols ABA abscisic acid - 9AA 9-aminoacridine - C, C K⁺ and Mg²⁺ concentrations giving equal relative fluorescence - F 9AA-fluorescence intensity - F_max maximum 9AA fluorescence - surface charge density The authors are grateful to Professor L.P. Popova (Institute of Plant Physiology, Sofia, Bulgaria) for continuous support. This work was supported in part by the Bulgarian Ministry of Science and High Education under research contract No. 519.     

Energy transfer in the light-harvesting complex II of Dunaliella tertiolecta is unusually sensitive to Triton X-100

Triton X-100, a detergent commonly used to solubilize higher plant thylakoid membranes, was found to be deleterious to Dunaliella LHC II. It disrupted the transfer of excitation energy from chlorophyll b to chlorophyll a. Based on analysis of pigments and immunoassays of LHC II apoproteins from sucrose density gradient fractions, Triton X-100 caused aggregation of the complex, but apparently did not remove chlorophyll b from the apoprotein. Following solubilization with Triton X-100 only CPI could be resolved by electrophoresis. In contrast, solubilization of Dunaliella thylakoids with octyl--D-glucopyranoside preserved energy transfer from chlorophyll b to chlorophyll a. This detergent also effectively prevented aggregation on sucrose gradients and preserved CPI oligomers, as well as LHCP1 and LHCP3 on non-denaturing gels. Solubilization with Deriphat gave similar results. We propose that room temperature fluorescence excitation and emission spectroscopy be used in conjunction with other biophysical and biochemical probes to establish the effects of detergents on the integrity of light harvesting chlorophyll protein complexes. Methods used here may be applicable to other chlorophytes which prove refractory to protocols developed for higher plants.Abbreviations LHC II light harvesting chlorophyll protein complex associated with photosystem II - LHCP1 and LHCP3 monomeric and oligomeric forms of LHC II, respectively, observed on non-denaturing gels - LiDS lithium dodecylsulphate - PMSF phenylmethylsulfonyl fluoride     

Characteristics of the Quenching of 9-Aminoacridine Fluorescence by Liposomes Made from Plant Lipids

Several laboratories have determined the surface charge density of membranes utilizing methods based on vesicle-induced quenching of the fluorescence of 9-aminoacridine and its relief by other cations. However, the computational methods by which surface charge density were calculated have not been verified in a model system. In this study, the quenching of 9-aminoacridine fluorescence by liposomes made from varying amounts of digalactosyldiacylglyceride and phosphatidic acid and relief of quenching by salts was examined. Quenching of 9-aminoacridine fluorescence increased with increasing amounts of phosphatidic acid added, independent of the composition of the added liposomes. In certain instances, the computational methods did not yield the surface charge density of the liposomes expected from their composition. However, when the effects of background ionic strength on surface potential were considered, there was a positive correlation between expected and calculated values. Therefore, the data support the contention that changes in the fluorescence of 9-aminoacridine can be used to calculate surface charge density of membranes. Received: 29 November 1999/Revised: 31 July 2000     

Light scattering and quenching of 9-aminoacridine fluorescence as indicators of the phosphorylation state of the adenylate system in intact spinach chloroplasts

Upon illumination of suspensions of intact chloroplasts, fluorescence of 9-aminoacridine was quenched, light scattering was increased, chlorophyll fluorescence was decreased after an initial increase, and chloroplast $\text{ATP}\text{ADP}$ ratios were increased. The response of 9-aminoacridine fluorescence quenching and light scattering to light intensity, anaerobiosis and inhibition of electron transport by DCMU was similar to that shown by chloroplast $\text{ATP}\text{ADP}$ ratios. It is discussed under what conditions 9-aminoacridine fluorescence quenching or light scattering can be used to monitor changes in the phosphorylation state of the chloroplast adenylate system.     

Further studies of the relationship between cation-induced chlorophyll fluorescence and thylakoid membrane stacking changes

Salt-induced changes in thylakoid stacking and chlorophyll fluorescence do not occur with granal membranes obtained by treatment of stacked thylakoids with digitonin. In contrast to normal untreated thylakoids, digitonin prepared granal membranes remain stacked under all ionic conditions and exhibit a constant high level of chlorophyll fluorescence. However, unstacking of these granal membranes is possible if they are pretreated with either acetic anhydride or linolenic acid.Trypsin treatment of the thylakoids inhibits the salt induced chlorophyll fluorescence and stacking changes but stacking of these treated membranes does occur when the pH is lowered, with the optimum being at about pH 4.5. This type of stacking is due to charge neutralization and does not require the presence of the 2000 dalton fragment of the polypeptide associated with the $\text{chlorophyll}\text{a}\text{chlorophyll}\text{b}$ light harvesting complex and known to be lost during treatment with trypsin (Mullet, J.E. and Arntzen, C.J. (1980) Biochim. Biophys. Acta 589, 100–117).Using the method of 9-aminoacridine fluorescence quenching it is argued that the surface charge density, on a chlorophyll basis, of unstacked thylakoid membranes is intermediate between digitonin derived granal and stromal membranes, with granal having the lowest value.The results are discussed in terms of the importance of surface negative charges in controlling salt induced chlorophyll fluorescence and thylakoid stacking changes. In particular, emphasis is placed on a model involving lateral diffusion of different types of chlorophyll protein complex within the thylakoid lipid matrix.     

Spectroscopy of non-photochemical and photochemical quenching of chlorophyll fluorescence in leaves; evidence for a role of the light harvesting complex of Photosystem II in the regulation of energy dissipation

Dissipation of absorbed excitation energy as heat, measured by its effect on the quenching of chlorophyll fluorescence, is induced under conditions of excess light in order to protect the photosynthetic apparatus of plants from light-dependent damage. The spectral characteristics of this quenching have been compared to that due to photochemistry in the Photosystem II reaction centre using leaves of Guzmania monostachia. This was achieved by making measurements at 77K when fluorescence emission bands from each type of chlorophyll protein complex can be distinguished. It was demonstrated that photochemistry and non-photochemical dissipation preferentially quench different emission bands and therefore occur by dissimilar mechanisms at separate sites. It was found that photochemistry was associated with a preferential quenching of emission at 688 nm whereas the spectrum for rapidly reversible non-photochemical quenching had maxima at 683 nm and 698 nm, suggesting selective quenching of the bands originating from the light harvesting complexes of Photosystem II. Further evidence that this was occurring in the light harvesting system was obtained from the fluorescence excitation spectra recorded in the quenched and relaxed states.Abbreviations pH transthylakoid pH gradient - F_o minimum level of chlorophyll fluorescence when Photosystem II reaction centres are open - F_m maximum level of fluorescence when Photosystem II reaction centres are closed - F_v variable fluorescence F_m minus F_o - F'_o F_o in any quenched state - F_m F_m in any quenched state - LHCII light harvesting complexes of Photosystem II - PSI Photosystem I - PS II Photosystem II - qN non-photochemical quenching of chlorophyll fluorescence - qE non-photochemical quenching of chlorophyll fluorescence that occurs in the presence of a pH     

Studies on 9-amino-6-chloro-2-methoxy acridine fluorescence quenching and enhancement in relation to energy transduction in spheroplasts and intact cells of the cyanobacterium Plectonema boryanum

The fluorescent probe 9-amino-6-chloro-2-methoxy acridine was used to study the energy transduction in the thylakoid and cell membranes of the cyanobacterium Plectonema boryanum. Apart from light-driven electron transfer, the dark endogenous respiration also leads to energization resulting in an ACMA fluorescence response, that is sensitive to the electron flow inhibitor 2, 5-dibromo-3-methyl-6-isopropyl-p-benzoquinone, to the energy transfer inhibitors dicyclohexylcarbodiimide and venturicidine and to the uncoupler 5-chloro-3-t-butyl-2-chloro-4-nitrosalicylanilide.In spheroplasts, in which the cell membranes have lost their capacity to maintain a proton gradient, the respiration-and light-induced ACMA fluorescence changes (quenching) are similar to those in chloroplasts. In intact cells a combination of reversible quenching and enhancement of ACMA fluorescence was found. This dualistic behaviour is supposedly caused by an opposite orientation of the thylakoid and cell membranes. ACMA quenching at the level of the thylakoids was obtained either by respiratory or photosynthetic electron transfer and gave similar responses to those obtained in the spheroplasts. The slower ACMA fluorescence enhancement, only observed in cells with intact cell membranes, also evoked by both respiration and light-induced energization is sensitive to the compounds mentioned above and in addition to KCN.Our results support the view [8] that dark oxidation of substrates by O₂ proceeds via the thylakoid membrane and terminates at a CN^- sensitive oxidase located in the cell membrane which requires the involvement of a mobile cytoplasmic redox mediator.Abbreviations ACMA 9-amino-6-chloro-2-methoxy acridine - chl a chlorophyll a - DBMIB 2, 5-dibromo-3-methyl-6-isopropyl-p-benzoquinone - DCCD dicyclohexylcarbodiimide - DNP dinitrophenol - DNP-INT dinitrophenyl ether of 2-iodo-4-nitrothymol - FCCP carbonylcyanide-p-trifluoro-methoxy phenylhydrazone - S-13 5-chloro-3-t-butyl-2-chloro-4-nitrosalicylanilide - tricine N-2 (2-Hydroxy-1, 1-bis (hydroxymethyl) ethyl)-glycine - Tris Tris (hydroxymethyl) amino methane     

Occurrence of the carotenoid lactucaxanthin in higher plant LHC II

The pigment composition of the light-harvesting complexes of Photosystem II (LHC II) has been determined for lettuce (Lactuca sativa). In common with other members of the composite, the photosynthetic tissues of this species may contain large amounts of the carotenoid lactucaxanthin (, -carotene-3,3'-diol) in addition to their normal compliment of carotenoids. The occurrence and distribution of lactucaxanthin in LHC II has been examined using isoelectric focusing of BBY particles followed by reversed-phase HPLC analysis of the pigments. The major carotenoids detected in LHC IIb, LHC IIa (CP29) and LHC IIc (CP26) purified from dark-adapted lettuce were lutein, violaxanthin, neoxanthin and lactucaxanthin. Lactucaxanthin has been shown to be a major component of PS II, accounting for 26% of total xanthophyll in both LHC IIb (23% total xanthophyll) and in the minor complexes (12–16%). In this study, LHC IIb was clearly resolved into four bands and their carotenoid composition determined. These four bands proved to be very similar in their pigment content and composition, although the relative amounts of neoxanthin and lutein in particular were found to increase from bands 1 to 4 (i.e. with increasing electrophoretic mobility). The operation of the xanthophyll cycle has also been examined in the LHC of L. sativa following light treatment. The conversion efficiency for violaxanthinzeaxanthin was nearly identical for each light-harvesting complex examined at 58–61%. Nearly half of the zeaxanthin formed in PS II was associated with LHC IIb, although the molar ratio of zeaxanthin:chlorophyll a was highest in the minor LHC.Abbreviations HPLC high performance liquid chromatography - IEF isoelectric focusing - LHCII light-harvesting complex associated with Photosystem II - PS II Photosystem II - qE pH-dependent nonphotochemical quenching of chlorophyll fluorescence