Changes in the redox state of the secondary acceptor of Photosystem II associated with light-induced thylakoid protein phosphorylation

Thylakoid membrane protein phosphorylation affects photochemical reactions of Photosystem II. Incubation of thylakoids in the light with ATP leads to: (1) an increase in the amplitude of three components (4–6, 25–45 and 280–300 μs) of delayed light emission after a single flash without any change in their kinetics; (2) a reduction of the flash-dependent binary oscillations of chlorophyll a fluorescence yield associated with electron transfer from the primary quinone acceptor, Q, to the secondary quinone acceptor, B; (3) an increase in the $\text{B}{}^{\mathrm{?}}\text{B}$ ratio resulting from an increase in stability of the semiquinone anion during dark adaptation; and (4) no change in the redox state of the plastoquinone pool as determined by flash-induced photooxidation of the Photosystem I reaction center, P-700. All the above observations are reversible upon dephosphorylation of the thylakoid membranes. These data are explained by a protein phosphorylation-induced stabilization of the bound semiquinone anion, B^?. It is proposed that this increased stability may be due to an alteration in the accessibility of an endogenous reductant to B, or to an increase in dissipative cycling of charge around Photosystem II.     

Analysis of chlorophyll fluorescence induction curves in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea as a function of magnesium concentration and NADPH-activated light-harvesting chlorophyll ab-protein phosphorylation

The effect of Mg²⁺ concentration and phosphorylation of light-harvesting chlorophyll $\text{a}\text{b-}\text{protein}$ on various chlorophyll fluorescence induction parameters of isolated pea thylakoids has been studied. (1) Lowering the Mg²⁺ concentration from 3 to 0.4 mM decreases only the variable fluorescence (F_v) and the area above the induction curve while at the same time increasing the slow exponential component of the rise (β_max). (2) A further decrease in Mg²⁺ concentration from 0.4 to 0 mM decreases the initial (F₀) fluorescence level such that the ratio $\text{F}{}_{\mathrm{<mtext>v</mtext>}}\text{F}{}_{\mathrm{<mtext>m</mtext>}}$ increases slightly as does the area above the induction curve and β_max. (3) Thylakoid membranes, phosphorylated at 5 mM Mg²⁺, show an equal decrease in F_v and F₀, no change in the area above the induction curve and an increase in β_max. At 2 mM Mg²⁺, however, phosphorylation induced a more extensive quenching of F_v so that the $\text{F}{}_{\mathrm{<mtext>v</mtext>}}\text{F}{}_{\mathrm{<mtext>m</mtext>}}$ ratio was lowered and the area above the induction curve decreased while β_max increased. (4) When phosphorylated membranes were subsequently suspended in an Mg²⁺-free medium the effect on F₀ due to phosphorylation was found to be additive to that due to the absence of Mg²⁺. The effect of membrane phosphorylation on fluorescence is discussed in relation to the control of excitation energy distribution and shows that different mechanisms operate depending on the background Mg²⁺ levels. At high Mg²⁺ the phosphorylation seems to affect the absorption cross-section of Photosystem II while at lower Mg²⁺ levels there is an additional effect of increased spillover from Photosystem II to I.     

Stimulation of microsecond-delayed fluorescence from spinach chloroplasts by uncouplers and by phosphorylation

Delayed fluorescence, as measured with a laser phosphoroscope, is stimulated not inhibited by uncouplers during the first 100 μs after the light is turned off. This is true only wen uncouplers cause an increase in the rate of electron transport. When ADP and P_i cause an increase in the electron transport rate, microsecond-delayed fluorescence is also increased. Indeed, there is a complex quantitative relationship between the rate of electron transport and the initial intensity of delayed fluorescence under a wide range of conditions.

Uncouplers or ADP and P_i also increase the rate of decay of delayed fluorescence so that after about 150 μs they become inhibitory, as already reported by many authors.

Microsecond-delayed fluorescence continues to rise with rising light intensities long after the rate of reduction of exogenous acceptor is light-saturated.

These observations suggest a correlation of the rate of electron transport both with the intensity of the 5–100 μs-delayed fluorescence and with the rate of decay in the intensity of delayed fluorescence. The data imply that the decrease in intensity of millisecond-delayed fluorescence which has often been noted with uncouplers is probably not due to the elimination of a membrane potential. It seems more likely that the decrease in millisecond-delayed fluorescence is a reflection of the rate of disappearance of some other electron transport-generated condition, a condition which is uncoupler-insensitive. Certainly stimulations of microsecond-delayed fluorescence by electron transport which has been uncoupled by gramicidin suggest that ion gradients are not an essential component of the conditions responsible for delayed fluorescence.     

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.     

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.     

The high-energy state of the thylakoid system as indicated by chlorophyll fluorescence and chloroplast shrinkage

Certain long-term fluorescence phenomena observed in intact leaves of higher plants and in isolated chloroplasts show a reverse relationship to light-induced absorbance changes at 535 nm (“chloroplast shrinkage”).

1. 1. In isolated chloroplasts with intact envelopes strong fluorescence quenching upon prolonged illumination with red light is accompanied by an absorbance increase. Both effects are reversed by uncoupling with cyclohexylammonium chloride.

2. 2. The fluorescence quenching is reversed in the dark with kinetics very similar to those of the dark decay of chloroplast shrinkage.

3. 3. In intact leaves under strong illumination with red light in CO₂-free air a low level of variable fluorescence and a strong shrinkage response are observed. Carbon dioxide was found to increase fluorescence and to inhibit shrinkage.

4. 4. Under nitrogen, CO₂ caused fluorescence quenching and shrinkage increase at low concentrations. At higher CO₂ levels fluorescence was increased and shrinkage decreased.

5. 5. In the presence of CO₂, the steady-state yield of fluorescence was lower under nitrogen than under air, whereas chloroplast shrinkage was stimulated in nitrogen and suppressed in air.

6. 6. These results demonstrate that the fluorescence yield does not only depend on the redox state of the quencher Q, but to a large degree also on the high-energy state of the thylakoid system associated with photophosphorylation.

Photoinduced quenching of chlorophyll fluorescence in intact chloroplasts and algae. Resolution into two components

The light-induced decline of chlorophyll a fluorescence from a peak (P) to a low stationary level (S) in intact, physiologically active isolated chloroplasts and in intact Chlorella cells is shown to be predominantly composed of two components: (1) fluorescence quenching by partial reoxidation of the quencher Q, the primary acceptor of Photosystem II and (2) energy-dependent fluorescence quenching related to the photoinduced acidification of the intrathylakoid space. These two mechanisms of fluorescence quenching can be distinguished by the different kinetics of the relaxation of quenching observed upon addition of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea (DCMU). The relaxation of quenching by addition of DCMU is biphasic. The fast phase with a half-time of about 1 s is attributed to the reversal of Q-dependent quenching. The slow phase with a half-time of about 15 s in chloroplasts and 5 s in Chlorella cells is ascribed to relaxation of energy-dependent quenching. As shown by fluorescence spectroscopy at 77 K, the energy-dependent fluorescence quenching essentially is not caused by increased transfer of excitation energy to Photosystem I. By analyzing the energy- and Q-dependent components of quenching, information on the energy state of the thylakoid membranes and on the redox state of Q under various physiological conditions is obtained.     

Characterization of chlorophyll fluorescence quenching in chloroplasts by fluorescence spectroscopy at 77 K II. ATP-dependent quenching

In intact, uncoupled type B chloroplasts from spinach, added ATP causes a slow light-induced decline ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{≈ 3}\text{min}$) of chlorophyll a fluorescence at room temperature. Fluorescence spectra were recorded after fast cooling to 77 K and normalized with fluorescein as an internal standard. Related to the fluorescence quenching at room temperature, an increase in Photosystem (PS) I fluorescence (F₇₃₅) and a decrease in PS II fluorescence (F₆₉₅) were observed in the low-temperature spectra. The change in the $\text{F}{}_{735}\text{F}{}_{695}$ ratio was abolished by the presence of methyl viologen. Fluorescence induction at 77 K of chloroplasts frozen in the quenched state showed lowered variable (F_v) and initial (F₀) fluorescence at 690 nm and an increase in F₀ at 735 nm. The results are interpreted as indicating an ATP-dependent change of the initial distribution of excitation energy in favor of PS I, which is controlled by the redox state of the electron-transport chain and, according to current theories, is caused by phosphorylation of the light-harvesting complex.     

The fluorescence decay kinetics of in vivo chlorophyll measured using low intensity excitation

We report fluorescence lifetimes for in vivo chlorophyll a using a time-correlated single-photon counting technique with tunable dye laser excitation. The fluorescence decay of dark-adapted chlorella is almost exponential with a lifetime of 490 ps, which is independent of excitation from 570 nm to 640 nm.Chloroplasts show a two-component decay of 410 ps and approximately 1.4 ns, the proportion of long component depending upon the fluorescence state of the chloroplasts. The fluorescence lifetime of Photosystem I was determined to be 110 ps from measurements on fragments enriched in Photosystem I prepared from chloroplasts with digitonin.     

Intensity effects on the fluorescence of in vivo chlorophyll

A technique for measuring relative quantum yields of fluorescence with a picosecond streak camera is described. We show that Chlorella pyrenoidosa exhibit an intensity dependent quantum yield when irradiated with single picosecond light pulses. This effect also occurs under conditions that inhibit the activity of the reaction centres, which can therefore be excluded as the cause.When a pulse train (pulse separation 6.9 ns) was used, the quantum yield was further reduced by the light absorbed from previous pulses, which indicates the formation of a quenching species having a relatively long lifetime.Absolute quantum yields calculated from the fluorescence decay show that single excitation pulses of 3 · 10¹³ photons/cm² give results comparable to those obtained by very low intensity methods.     

Interactions of herbicides and azidoquinones at a Photosystem II binding site in the thylakoid membrane

6-Azido-5-decyl-2,3-dimethoxy-p-benzoquinone (6-azido-Q₀C₁₀) was found to replace the native plastoquinone at B (the second stable electron acceptor to Photosystem II (PS II)). The 6-azido-Q₁₀C₁₀ would accept electrons from the primary electron-accepting quinone, Q, thus allowing electron transport through PS II to the plastoquinone pool in thylakoids. The synthetic azidoquinone also competes with the PS II herbicides ioxynil and atrazine for binding. This observation strongly favors the hypothesis that PS II herbicides block electron transport by replacing the native quinone which acts as the second electron carrier on the reducing side of PS II (termed B). Covalent linkage of 6-azido-Q₀C₁₀ to its binding environment by ultraviolet irradiation greatly reduces herbicide-binding affinity but does not lead to a loss in herbicide-binding sites. We take this as evidence that covalent attachment of 6-azido-Q₀C₁₀ allows some freedom of quinone head-group movement such that the herbicides can enter the binding site. This indicates that the protein determinants which regulate quinone and herbicide binding are very closely related, but not identical. A compound somewhat related to 6-azido-Q₀C₁₀ is 2-azido-3-methoxy-5-geranyl-6-methyl-p-benzoquinone (2-azido-Q₂). This compound was found to be an ineffective competitor with respect to herbicide binding. Thus, interactions with protein-binding determinants are highly dependent on the molecular structure of quinones. The 2-azido-Q₂ was an inhibitor of electron flow in the intersystem portion of the chain.     

Thylakoid conformational changes accompanying membrane protein phosphorylation

The effect of reversible membrane phosphorylation on the room temperature linear dichroism signal of magneto-oriented pea thylakoids was investigated. Membrane phosphorylation, induced by photoreduction of the plastoquinone pool, resulted in a change in the linear dichroism signal in the region of the red absorption band of chlorophyll. The optical change was due to modifications in selective polarized light scattering which have been shown to be indicative of alterations in the degree of membrane stacking. No changes in linear dichroism due to a reorientation of pigments were observed. It is concluded that phosphorylation of the membrane results in about a 10% destacking of the thylakoids and that this conformational change is implicated in energy redistribution between the two photosystems.     

On the nature of the fluorescence decrease due to phosphorylation of chloroplast membrane proteins

1. Phosphorylation of chloroplast membranes by illumination in the presence of ATP results in a 15–20% increase in the rate of Photosystem I electron transfer at low light intensity. 2. Phosphorylated membranes when depleted of Mg²⁺ and resuspended in a low salt medium still show a 17% lower yield of Photosystem II fluorescence than do unphosphorylated membranes. A 31% difference is seen after restoration of the maximal yield by addition of Mg²⁺. 3. The concentration of Mg²⁺ required to induce a half-maximal increase in fluorescence is 0.9 mM for control and 1.8 mM for phosphorylated chloroplasts. Phosphorylation at 1 mM Mg²⁺ can therefore cause more than double the amount of decrease in fluorescence yield from Photosystem II compared to phosphorylation at 5 mM. 4. The above results are discussed in terms of the mechanism of the ATP-induced fluorescence changes and a suggestion is made that the apparent interaction between phosphorylation and Mg²⁺ concentration may be a physiologically important phenomenon.     

The role of pH and membrane potential in the reactions of Photosystem II as measured by effects on delayed fluorescence

(1) If DCMU is added to chloroplasts which have been preilluminated (0–8 flashes) the turnover of the water-splitting enzyme is limited to one further transition upon continuous illumination. (2) The intensity of millisecond delayed fluorescence measured in the presence of mediators of cyclic electron transport around Photosystem I and of DCMU added after pre-flashing is stimulated above the level in the presence of DCMU alone and varies according to the number of pre-flashes (Bowes, J.M. and Crofts, A.R. (1978) Z. Naturforsch 33c, 271–275). (3) Separate contributions of the following energetic terms to the induction kinetics and extent of millisecond delayed fluorescence under these conditions have been examined with a view to assessing their involvement in and the mechanism of the stimulation of the emission above the level in dark-adapted chloroplasts in the presence of DCMU: (a) the initial pH of the phase in equilibrium with the water-splitting enzyme; (b) the change in internal pH which occurred when Photosystem I acted as a proton pump; (c) the electrical potential difference across the membrane resulting from rapid charging of the membrane capacitance. (4) It was confirmed that delayed light was stimulated as a result of the interaction of the intrathylakoid pH (3a and b) with the equilibria of the S-states involving proton release according to the model in which this occurs on all except the transition S₁ → S₂; the stimulation was qualitatively proportional to the number of protons released. (5) There was no marked variation of the membrane potential as a function of the number of pre-flashes.     

A study on the lateral distribution of the plastoquinone pool with respect to Photosystem II in stacked and unstacked spinach chloroplasts

The quenching of Photosystem II (PS II) chlorophyll fluorescence by oxidised plastoquinone has been used in an attempt to determine their relative distribution in the partition zone and stroma-exposed thylakoid membranes. Thus, the PS II-plastoquinone interaction was determined in stacked (2.5 mM MgCl₂) and largely unstacked (0.25 mM MgCl₂) membranes. A method to correct for spillover or other quenching changes at the different MgCl₂ concentrations, which would compete with the plastoquinone-induced quenching, was devised utilising the quinone dibromothymoquinone. This compound is demonstrated to behave as an ideal (theoretically) PS II quencher at both high and low MgCl₂ concentrations, which indicates that it distributes itself homogeneously between partition zone and stroma-exposed membrane regions. In passing from the stacked to the unstacked configuration, the PS II-plastoquinone interaction decreases less than the PS II-dibromothymoquinone interaction. This is interpreted to mean that plastoquinone is present in both the partition zone and stroma-exposed membranes, with somewhat higher concentrations in the stroma-exposed membranes. Thus, plastoquinone is well placed to transport reducing equivalents from the partition zones to the stroma-exposed membranes.     

A quantitative determination of photochemical and non-photochemical quenching during the slow phase of the chlorophyll fluorescence induction curve of bean leaves

Estimations of the changes in the reduction-oxidation state of Photosystem II electron acceptors in Phaseolus vulgaris leaves were made during the slow decline in chlorophyll fluorescence emission from the maximal level at P to the steady-state level at T. The relative contributions of photochemical and non-photochemical processes to the fluorescence quenching were determined from these data. At a low photon flux density of 100 μmol · m^?2 · s^?1, non-photochemical quenching was the major contributor to the fluorescence decline from P to T, although large charges were observed in photochemical quenching immediately after P. On increasing the light intensity 10-fold, the contribution of photochemical processes to fluorescence quenching was markedly diminished, with nearly all the P-to-T fluorescence decline being attributable to changes in non-photochemical quenching. The possible factors responsible for changes in non-photochemical quenching within the leaves are discussed.     

The influence of the electric diffusion potential on delayed fluorescence light curves of chloroplasts treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea

The potassium salt-induced transient increase of delayed fluorescence yield was studied in pea chloroplasts treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea.A simple kinetic model is proposed to account for the actinic light intensity dependence of the delayed fluorescence enhancement by the transmembrane diffusion potential induced by sudden salt addition. The electric field dependence of the rate constants for the recombination of primary separated charges with and without subsequent electronic excitation of reaction center chlorophyll was obtained.From the value of enhancement of delayed fluorescence by salt concentration gradients at saturating actinic light intensity, it is concluded that the distance, normal to thylakoid membrane surface, between the primary acceptor and the donor of Photosystem II is smaller than the membrane thickness.     

Picosecond fluorescence kinetics in spinach chloroplasts at room temperature. Effects of phosphorylation

We have used single-photon timing with picosecond resolution to investigate the effect of phosphorylation on the fluorescence decay from broken spinach chloroplasts. Phosphorylation of spinach thylakoids causes a quenching of the slow decay phase (equivalent to a quenching of variable fluorescence) and an increase in the yield of the middle phase decay component. In addition, phosphorylation alters the intensity dependence of fluorescence in a manner which indicates a decreased antenna size of Photosystem II. The observed changes are indicative of a State 1-State 2 transition and show a clear reversal when the membranes are dephosphorylated.