The reduction of the oxygen-evolving system in chloroplasts by thylakoid components

Using thoroughly dark-adapted thylakoids and an unmodulated Joliot-type oxygen electrode, the following results were obtained. (i) At high flash frequency (4 Hz), the oxygen yield at the fourth flash (Y₄) is lower compared to Y₃ than at lower flash frequency. At 4 Hz, the calculated S₀ concentration after thorough dark adaptation is found to approach zero, whereas at 0.5 Hz the apparent $\text{S}{}_0\text{(}\text{S}{}_0\text{+}\text{S}{}_1\text{)}$ ratio increases to about 0.2. This is explained by a relatively fast donation ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 1.0–1.5}\text{s}$) of one electron by an electron donor to S₂ and S₃ in 15–25% of the Photosystem II reaction chains. The one-electron donor to S₂ and S₃ appears to be rereduced very slowly, and may be identical to the component that, after oxidation, gives rise to ESR signal II_s. (ii) The probability for the fast one-electron donation to S₂ and S₃ has nearly been the same in triazine-resistant and triazine-susceptible thylakoids. However, most of the slow phase of the S₂ decay becomes 10-fold faster ($\text{t}{}_{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}\text{= 5–6}\text{s}$) in the triazine-resistant ones. In a small part of the Photosystem II reaction chains, the S₂ decay was extremely slow. The S₃ decay in the triazine-resistant thylakoids was not significantly different from that in triazine-susceptible thylakoids. This supports the hypothesis that S₂ is reduced mainly by Q^?_A, whereas S₃ is not. (iii) In the absence of CO₂/HCO^?_A and in the presence of formate, the fast one-electron donation to S₂ and S₃ does not occur. Addition of HCO^?₃ restores the fast decay of part of S₂ and S₃ to almost the same extent as in control thylakoids. The slow phase of S₂ and S₃ decay is not influenced significantly by CO₂/HCO^?₃. The chlorophyll a fluorescence decay kinetics in the presence of DCMU, however, monitoring the Q^?_A oxidation without interference of Q_B, were 2.3-fold slower in the absence of CO₂/HCO^?₃ than in its presence. (iv) An almost 3-fold decrease in decay rate of S₂ is observed upon lowering the pH from 7.6 to 6.0. The kinetics of chlorophyll a fluorescence decay in the presence of DCMU are slightly accelerated by a pH change from 7.6 to 6.0. This indicates that the equilibrium Q^?_A concentration after one flash is decreased (by about a factor of 4) upon changing the pH from 7.6 to 6.0. When direct or indirect protonation of Q^?_B is responsible for this shift of equilibrium Q^?_A concentration, these data would suggest that the pK_a value for Q^?_B protonation is somewhat higher than 7.6, assuming that the protonated form of Q^?_B cannot reduce Q_A.     

Preparation of O2-evolving Photosystem-II subchloroplasts from spinach

An O₂-evolving Photosystem II subchloroplast preparation was obtained from spinach chloroplasts, using low concentrations of digitonin and Triton X-100. The preparation showed an O₂ evolution activity equivalent to 20% of the uncoupled rate of fresh broken chloroplasts, but had no significant Photosystem-I-dependent O₂ uptake activity. The preparation showed a chlorophyll $\text{a}\text{b}$ ratio of 1.9 and a $\text{P-700}\text{chlorophyll}$ ratio of $\text{1}\text{2400}$. Absorption spectra at room temperature and fluorescence emission spectra of chlorophyll at 77 K suggested a significant decrease in Photosystem I antenna chlorophylls in the O₂-evolving Photosystem II preparation.     

Iodination of chloroplasts. I. Properties of iodinated chloroplasts

Spinach chloroplasts exposed to iodide can be washed free of the bulk of the iodide. In the presence of lactoperoxidase and H₂O₂, iodide can be introduced into chloroplasts in high amounts and in non diffusible forms. The resultant particles, which have been named iodochloroplasts, extrude their iodide upon stimulation by light. The form and the amount of extruded iodide bears a definite relationship to the amount of incident light. A flash of marginally effective light is additive to the next such flash even after a lapse of 10 min of darkness. These and other properties of iodochloroplasts may make them of great use in the study of intermediate reactions of photosynthesis.     

External electric field effects on prompt and delayed fluorescence in chloroplasts

An electric field pulse was applied to a suspension of osmotically swollen spinach chloroplasts after illumination with a saturating flash in the presence of DCMU. In addition to the stimulation of delayed fluorescence by the electric field, discovered by Arnold and Azzi (Arnold, W.A. and Azzi, R. (1971) Photochem. Photobiol. 14, 233–240) a sudden drop in fluorescence yield was observed. The kinetics of this fluorescence change were identical to those of the integrated delayed fluorescence emission induced by the pulse. The S-state dependence of the stimulated emission was very similar to that of the normal luminescence. We assume that the membrane potential generated by the pulse changes the activation energy for the back reaction in Photosystem II. On this basis, and making use of data we obtained earlier from electrochromic absorbance changes induced by the pulse, the kinetics of the field-induced prompt and delayed fluorescence changes, and also the amplitude of the fluorescence decrease, which was about 12% for a nearly saturating pulse, are explained. Our results indicate that in those reaction centers where a decrease of the activation energy occurs the effect of a pulse can be quite spectacular: the back reaction, which normally takes seconds, is completed in a few hundred microseconds when a sufficiently strong pulse is applied. Measurements of the polarization of the stimulated luminescence supported the interpretation given above.Only 2.8% of the back reaction was found to proceed via transition of reexcited chlorophyll to the ground state, both during the field pulse and in the absence of the field.     

Regulation of photosystem stoichiometry,chlorophyll a and chlorophyll b content and relation to chloroplast ultrastructure

The structural-functional organization of higher plant chloroplasts has been investigated in relation to the particular light conditions during plant growth. (1) Light intensity variations during growth caused changes in the $\text{Chl}\text{a}\text{Chl}\text{b}$ ratio, in the light-saturated uncoupled rates of electron transport to a Hill oxidant and in the distribution of the chloroplast volume between the membrane and stroma phases. (2) Light quality differences during growth had an effect on the PS II/PS I reaction center ratio and on the chloroplast membrane phase differentiation into grana and stroma thylakoids. Plants grown under far-red-enriched (680–710 nm) illumination contained higher (20–25%) amounts of PS II and simultaneously lower (20–25%) amounts of PS I reaction centers. They also showed a higher grana density along with thicker grana stacks in their chloroplasts. (3) The size of the light-harvesting antenna pool of PS II centers was estimated from the fluorescence time course of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea-poisoned chloroplasts and was found to be fairly constant (±10%) in spite of the variable PS II/PS I reaction center ratio. The results are compatible with the hypothesis that the structural entities of grana facilitated the centralization and relative concentration increase of a certain group of PS II reaction centers.     

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.     

The I-D fluorescence transient. An indicator of rapid energy distribution changes in photosynthesis

The I-D transient in the chlorophyll fluorescence induction curve (Kautsky effect) is investigated in the view of recently discovered rapid changes in energy distribution between the two photosystems (Schreiber, U. and Vidaver, W., FEBS Lett., in the press). Fluorescence induction curves differ appreciably depending on whether measured at λ < 690 nm, originating in pigment system II, or at λ > 715 nm, which is in part from pigment system I. The differences occur as well in the rapid part of the induction curve (O-I-D-P) as in the slower P-S decay. Most significant changes in energy distribution are indicated in the region of the I-D dip, being induced by appropriate preillumination. The effect is studied by (a) comparing the individual fluorescence time courses at λ < 690 nm and λ > 715, (b) plotting F < 690 vs. F > 715 and (c) recording time courses of $\text{F < 690}\text{F > 715}$ ratios. In (a) the I and D characteristics are delayed at F > 715 relative to F < 690, which is accompanied by periods close to I and D, where the two emissions follow inverse courses. In (b) the I-D dip corresponds to a loop. And in (c) it is shown that a rapid ratio decay, reflecting increasing excitation of System I pigments, is initiated before the I-D dip. These data indicate that the I-D transient is caused by a rapid switch of energy distribution in favor of System I and the resulting stimulation of Q reoxidation via the electron transport chain. It is suggested that as with the slow fluorescence transients the rapid also can be understood as a composite of two different changes, (1) direct changes resulting from a switch in energy distribution, which are inverse for F < 690 and F > 715, and (2) indirect changes due to stimulated Q reduction or Q oxidation, which are parallel for both emissions. The rapid ratio decay, correlated to I-D, persists and is even stimulated in the presence of electron transport inhibitors. This and the speed of the phenomenon make it improbable that the rapid energy distribution changes are affected by an ion flux-induced mechanism. It is proposed that the electrical field across the thylakoid membrane is involved in the energy switch mechanism.     

Effect of NADP+ on light-induced cytochrome changes in membrane fragments from a blue-green alga

The effect of NADP⁺ on light-induced steady-state redox changes of membrane-bound cytochromes was investigated in membrane fragments prepared from the blue-green algae Nostoc muscorum (Strain 7119) that had high rates of electron transport from water to NADP⁺ and from an artificial electron donor, reduced dichlorophenolindophenol (DCIPH₂) to NADP⁺. The membrane fragments contained very little phycocyanin and had excellent optical properties for spectrophotometric assays. With DCIPH₂ as the electron donor, NADP⁺ had no effect on the light-induced redox changes of cytochromes: with or without NADP⁺, 715- or 664-nm illumination resulted mainly in the oxidation of cytochrome f and of other component(s) which may include a c-type cytochrome with an α peak at 549 nm. With 664 nm illumination and water as the electron donor, NADP⁺ had a pronounced effect on the redox state of cytochromes, causing a shift toward oxidation of a component with a peak at 549 nm (possibly a c-type cytochrome), cytochrome f, and particularly cytochrome b₅₅₉. Cytochrome b₅₅₉ appeared to be a component of the main noncyclic electron transport chain and was photooxidized at physiological temperatures by Photosystem II. This photooxidation was apparent only in the presence of a terminal acceptor (NADP⁺) for the electron flow from water.     

Quantum efficiency and antenna size of Photosystems IIα, IIβ and I in tobacco chloroplasts

Reaction center concentrations were determined in chloroplasts of tobacco, cv John William's Broadleaf, and its mutants Su/su and Su/su var. Aurea. Quantum yields of the primary reactions of Photosystems I, II_α and II_β (Melis, A. and Homann, P.H. (1975) Photochem. Photobiol. 21, 431–437) were obtained by measurement of their rate constants and the absorbed energy, under conditions where all three photosystems operated simultaneously and produced almost irreversibly a single charge separation.The concentrations and reaction rates of the photosystems were different in chloroplasts from the wild type and the mutants, but in chloroplasts of each type of plant used essentially all quanta absorbed by chlorophyll caused a charge separation in PS I, PS II_α or PS II_β. Since the quantum efficiency of each photosystem was close to one, kinetic differences between the photosystems and between different kinds of chloroplasts were only due to differences in antenna size. From the rate constants the number of chlorophyll molecules in the antenna of each photosystem could be calculated. It is argued that PS II_α and PS II_β must be different, independent structures.     

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.     

Photoconversion kinetics of chloroplast Photosystems I and II. Effect of Mg2+

The effect of divalent cations on the primary photoconversion kinetics of chloroplast Photosystems (PS) I and II was investigated by absorbance difference spectrophotometry in the ultraviolet (ΔA₃₂₀) and red (ΔA₇₀₀) regions and by fluorescence at room temperature. Three main chlorophyll (Chl) a fluorescence emission components were identified. Addition of 5 mM MgCl₂ to unstacked chloroplasts caused a 5–7-fold increase in F_vα, the variable fluorescence yield controlled by the α-centers. The fluorescence yield F_vβ controlled by the β-centers and the nonvariable fluorescence yield F₀ were only slightly changed by the treatment. The absolute number of α- and β-centers remained unchanged and independent of divalent cations. The rate constants K_α, K_β and K_P-700 determined from the photoconversion kinetics of Q_α, Q_β and P-700 were also unchanged by divalent cations, suggesting a constancy of the respective absorption cross-sections. Evidence is presented that the Mg²⁺ effect on Chl a fluorescence is not due simply to unstacking. Conclusion: (1) In the absence of divalent cations from the chloroplast suspending medium, the variable fluorescence yield is not complementary to the rate of PS II photochemistry. (2) A spillover of excitation from PS II to PS I in the absence of Mg²⁺ cannot account for the 7-fold lowering of the variable fluorescence yield F_vα at room temperature. The results are discussed in view of a model of excitation transfer and fluorescence emission in the pigment bed of PS II_α and PS II_β.     

Chlorophyll composition of Photosystems IIα, IIβ and I in tobacco chloroplasts

The antenna composition of the Photosystems II_α, II_β and I was studied in tobacco chloroplasts. Absorbance spectra, recorded at 4 K, were analyzed for the wild type and the mutants Su/su and Su/su var. Aurea, containing higher concentrations of the photosystems. With chloroplasts of Su/su we measured the action spectra of the three photosystems from 625 to 690 nm. Above 675 nm absorption by Photosystem I dominated. This sytem had a maximum at 678 nm and a shoulder at 660 nm. Of the long-wavelength chlorophyll a forms, absorbing at 690, 697 and 705 nm at 4 K, which are generally assigned to Photosystem I, the 697 nm form occurred in an amount of four molecules per reaction center of Photosystem I in each type of chloroplast. The Photosystem II_α spectrum was characterized by maxima at 650 and 672 nm, showing clearly the participation of the chlorophyll a and b containing light-harvesting complex. In the mutants the light-harvesting complex has a chlorophyll a to chlorophyll b ratio of more than 1; the amount of the 672 nm chlorophyll a was normal, whereas the amount of chlorophyll b was markedly decreased in the mutants relative to the wild type. The Photosystem II_β spectrum mainly consisted of a band at 683 nm.     

Kinetic study of oxygen evolution parameters in tris-washed,reactivated chloroplasts

Tris-washed chloroplasts which have lost the ability to evolve oxygen can be reactivated by the procedure of Yamashita. T., Tsuji, J. and Tomita, G. ((1971)Plant Cell Physiol. 12, 117–126) [7] to give 100% of the rate of control chloroplasts in continuous illumination. Furthermore, in flashing light the reactivated chloroplasts exhibit oxygen-yield oscillations of period four that are characteristic of the control. Similar kinetic parameters for intermediate steps in the water-splitting process are observed for the two preparations. We conclude that the reactivation procedure restores the native oxygen evolution mechanism to Tris-washed chloroplasts.A relatively rapid and reversible (0.5 s decay) light-induced component of EPR Signal II is observed upon inhibition of O₂ evolution by Tris washing (Babcock G. T. and Sauer, K. (1975) Biochim. Biophys. Acta 376, 315–328) [10]. Reactivated chloroplasts are similar to untreated chloroplasts in that this Signal II transient is not observed. Manganese, which is released by Tris treatment to the interior of the thylakoid membrane in an EPR-detectable state, is returned to an EPR-undetectable state by reactivation. The reactivation procedure does not require light to restore O₂ evolution and EDTA has no effect on the extent of reactivation. These results are discussed in terms of possible mechanisms for manganese incorporation into photosynthetic membranes.     

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.     

Measurement of the relative electron-transport capacity of Photosystem I and Photosystem II in spinach chloroplasts

The ratio of Photosystem (PS) II to PS I electron-transport capacity in spinach chloroplasts was compared from reaction-center and steady-state rate measurements. The reaction-center electron-transport capacity was based upon both the relative concentrations of the PS II_α, PS II_β and PS I centers, and the number of chlorophyll molecules associated with each type of center. The reaction-center ratio of total PS II to PS I electron-transport capacity was about 1.8:1. Steady-state electron-transport capacity data were obtained from the rate of light-induced absorbance-change measurements in the presence of ferredoxin-NADP⁺, potassium ferricyanide and 2,5-dimethylbenzoquinone (DMQ). A new method was developed for determining the partition of reduced DMQ between the thylakoid membrane and the surrounding aqueous phase. The ratio of membrane-bound to aqueous DMQH₂ was experimentally determined to be 1.3:1. When used at low concentrations (200 μM), potassium ferricyanide is shown to be strictly a PS I electron acceptor. At concentrations higher than 200 μM, ferricyanide intercepted electrons from the reducing side of PS II as well. The experimental rates of electron flow through PS II and PS I defined a PS II/PS I electron-transport capacity ratio of 1.6:1.