Charge accumulation and recombination in Photosystem II studied by thermoluminescence. I. Participation of the primary acceptor Q and secondary acceptor B in the generation of thermoluminescence of chloroplasts

In the glow curves of chloroplasts excited by a series of flashes at +1°C the intensity of the main thermoluminescence band appearing at +30°C (B band; B, secondary acceptor of Photosystem II) exhibits a period-4 oscillation with maxima on the 2nd and 6th flashes indicating the participation of the S₃ state of the water-splitting system in the radiative charge recombination reaction. After long-term dark adaptation of chloroplasts (6 h), when the major part of the secondary acceptor pool (B pool) is oxidized, a period-2 contribution with maxima occurring at uneven flash numbers appears in the oscillation pattern. The B band can even be excited at ?160°C as well as by a single flash in which case the water-splitting system undergoes only one transition (S₁ → S₂). The experimental observations and computer simulation of the oscillatory patterns suggest that the B band originates from charge recombination of the S₂B^? and S₃B^? redox states. The half-time of charge recombination responsible for the B band is 48 s. When a major part of the plastoquinone pool is reduced due to prolonged excitation of the chloroplasts by continuous light, a second band (Q band; Q, primary acceptor of Photosystem II) appears in the glow curve at +10°C which overlaps with the B band. In chloroplasts excited by flashes prior to DCMU addition only the Q band can be observed showing maxima in the oscillation pattern at flash numbers 2, 6 and 10. The Q band can also be induced by flashes after DCMU addition which allows only one transition of the water-splitting system (S₁ → S₂). In the presence of DCMU, electrons accumulate on the primary acceptor Q, thus the Q band can be ascribed to the charge recombination of either the S₂Q^? or S₃Q^? states depending on whether the water-splitting system is in the S₂ or the S₃ state. The half-time of the back reaction of Q^? with the donor side of PS II (S₂ or S₃ states) is 3 s. It was also observed that in a sequence of flashes the peak positions of the Q and B bands do not depend on the advancement of the water-splitting system from the S₂ state to the S₃ state. This result implies that the midpoint potential of the water-splitting system remains unmodified during the S₂ → S₃ transition.     

Thermoluminescence study of charge recombination in Photosystem II at low temperatures. II. Oscillatory properties of the Zv and A thermoluminescence bands in chloroplasts dark-adapted for various time periods

The oscillations of the Z_V and A thermoluminescence bands were investigated in spinach chloroplasts which had been dark-adapted for various time periods and subjected to a series of flashes at +2°C before continuous illumination at various low temperatures. When excited with continuous light below −65°C, the Z_V band exhibited period-4 oscillation, with maxima on preflashes 0, 4 and 8. Above −65°C, the oscillation pattern depended greatly on the dark-adaptation period of the chloroplasts. In preilluminated samples (15 s light followed by 3 min dark), when the Q_B pool is half oxidized, the oscillation of the thermoluminescence intensity measured at −50°C was similar to that observed below −65°C. However, after the thorough dark-adaptation of the chloroplasts (6 h), when the major fraction of the Q_B pool is assumed to be oxidized, a binary oscillation appeared in the oscillation pattern, with maxima at odd flash numbers. Below −65°C, period-2 oscillation of the Z_V band could not be induced by the dark-adaptation of the chloroplasts, suggesting an inhibition of electron exchange between Q_A and Q_B. Upon excitation of the chloroplasts with continuous light at −30°C, the A band oscillated with a periodicity of 4 with maxima at preflash numbers 2 and 6. At pH 7.5, the period-4 oscillation was converted into a period-2 oscillation by thorough dark-adaptation of the chloroplasts (24 h). Model calculations of the oscillatory patterns suggest that the period-4 oscillations of the Z_V and A bands are determined by the concentrations [S₀] + [S₁] and [S₂] + [S₃], respectively, which are present after the preflashes prior to the low-temperature continuous illumination. The period-2 oscillations in the amplitudes of the Z_V and A bands reflect the changes occurring in the redox state of the Q_B pool in a sequence of flashes. The possible relationship between the characteristics of the Z_V and A bands and the temperature-dependence of the S state transitions was investigated. Comparison of the amplitudal changes of the B (S₂Q⁻_B and S₃Q⁻_B recombination) and Q (S₂Q⁻_A recombination) thermoluminescence bands as a function of the excitation temperature suggests that the S₂ → S₃ and S₃ → S₄ transitions are blocked at about −65 and −40°C, respectively. It is also concluded that the thermoluminescence intensity emitted by the reaction center is about twice as high in the S₃ state as in the S₂ state.     

Interaction of 1,4-benzoquinones with Photosystem II in thylakoids and Photosystem II membrane fragments from spinach

The interaction of exogenous quinones with the Photosystem II (PS II) acceptor side has been analyzed by measurements of flash-induced 320 nm absorption changes, transient flash-induced variable fluorescence changes, thermoluminescence emission and oxygen yield in dark-adapted thylakoids and PS II membrane fragments. Two classes of 1,4-benzoquinones were shown to give rise to remarkably different reaction patterns. (A) Phenyl-p-benzoquinone (Ph-p-BQ) -type compounds give rise to a marked binary oscillation of the initial amplitudes of 320 nm absorption changes induced by a flash train in dark-adapted PS II membrane fragments and a retardation of the decay kinetics of the flash-induced variable fluorescence. The electron transfer reactions to these type of quinones are severely inhibited by 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU). (B) In the presence of tribromotoluquinone (TBTQ) a different oscillation pattern of the 320 nm absorption changes is observed characterized by a marked relaxation after the first flash in the 5 ms domain. This relaxation is insensitive to 10 μM DCMU. Likewise the decay of the flash-induced variable fluorescence in TBTQ-treated samples is much less sensitive to DCMU than in control. The thermoluminescence emission exhibits an oscillation in samples incubated for 5 min with TBTQ before addition of 30 μM DCMU. Under the same conditions a significant flash-induced oxygen evolution is observed only after the third and fourth flash, respectively, whereas in the presence of TBTQ alone a normal oscillation pattern is observed. The different functional patterns of PS II caused by the two types of classes of exogenous quinones are interpreted by their binding properties: a noncovalent association with the Q_B-site of Ph-p-BQ-type quinones versus a tight (covalent?) binding in the vicinity of Q_A (possibly also at the Q_B-site) in the case of halogenated 1,4-benzoquinones. The mechanistic implications of these findings are discussed.     

Light-induced changes of fluorescence and absorbance in spinach chloroplasts at −40 °C

1. 1. Spinach chloroplasts were stored in the dark for at least 1 h, rapidly cooled to −40 °C, and illuminated with continuous light or short saturating flashes. In agreement with the measurements of Joliot and Joliot, chloroplasts that had been preilluminated with one or two flashes just before cooling showed a less efficient increase in the yield of chlorophyll a fluorescence upon illumination at −40 °C than dark-adapted chloroplasts. The effect disappeared below −150 °C, but reappeared again upon warming to −40 °C. Little effect was seen at room temperature in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), added after the preillumination.

2. 2. Light-induced absorbance difference spectra at −40 °C in the region 500–560 nm indicated the participation of two components, the socalled 518-nm change (P518) and C-550. After preillumination with two flashes the absorbance change at 518 nm was smaller, and almost no C-550 was observed. After four flashes, the bands of C-550 were clearly visible again.

3. 3. The fluorescence increase and the absorbance change at 518 nm showed the same type of flash pattern with a minimum after the second and a maximum at the fourth flash. In the presence of 100 μM hydroxylamine, the fluorescence response was low after the fourth and high again after the sixth flash, which confirmed the hypothesis that the flash effect was related to the so-called S-state of the electron transport pathway from water to Photosystem 2.

4. 4. The kinetics of the light-induced absorbance changes were the same at each wavelength, and, apart from the size of the deflection, they were independent of preillumination. Flash experiments indicated that the absorbance changes were a one-quantum reaction. This was also true for the fluorescence increase in dark-adapted chloroplasts, but with preilluminated chloroplasts several flashes were needed to approximately saturate the fluorescence yield.

5. 5. The results are discussed in terms of a mechanism involving two electron donors and two electron acceptors for System 2 of photosynthesis.

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.     

Degradation of Storage Photosynthates in Isolated Spinach Mesophyll Cells in CO2-Free System and Its Regulatory Factors

Isolated spinach (spinacia oleracea L.) mesophyll cells, after being preilluminated for 40 min for storage photosynthates loading (14C), were shifted into CO2-free mixture for investigation of storage photosynthates degradation and its regulatory factors. The loss of fixed carbon (14C) after 30 min incubation in CO2-free mixture in light was about 20%, which was much higher than that in dark (about 4.5%). The loss of fixed carbon was apparently stimulated by the increase of light intensity or O2 concentration and depressed by DCMU or NH4C1. Moreover, the loss of fixed carbon, especially the soluble fraction, was reduced by the addition of glycolate in light but not in dark. The obvious degradation of starch in spinach mesophyll cells in CO2-free system was monitored both in light and in dark. Unlike in dark, starch degradation in light was not associated with a detectable accumulation of the soluble products (PGA, Ribulose5-phosphate, sucrose etc.). Based on the above results, the different metabolic patterns for the products of starch degradation in light and in dark were discussed and the possible physiological roles were also proposed.     

Thermoluminescence study of charge recombination in Photosystem II at low temperatures. I. Characterization of the Zv and A thermoluminescence bands

The characteristics of the Z_v and A thermoluminescence bands appearing in the glow curve at about -75 and -30°C, respectively, were investigated in spinach chloroplasts. Inhibitory concentrations of DCMU decreased the amplitude of the Z_v band by half and completely abolished the A band. On the other hand, after two preflashes at +2°C before freezing, the A band could be charged by low-temperature illumination even when the electron transport was interrupted between Q_A and Q_B by DCMU addition after the preflashes. Two-flash preillumination greatly enhanced the amplitude of the A band, but diminished that of the Z_v band. Tris washing and NH₂OH treatment, which inactivated the oxygen-evolving system, almost completely abolished the Z_v band, but did not affect the A band. Severe trypsin treatment, which also impaired the oxygen-evolving system, resulted in a very large intensification of the Z_v band. The half-times of the A and Z_v bands, determined by theoretical analysis of the thermoluminescence data, proved to be about 4 ms and 200–500 μs, respectively. These results, taken together with EPR data from the literature, suggest that the A band arises from charge recombination between a negatively charged acceptor located before the DCMU block (most probably Q⁻_A) and the oxidized donor Z⁺ (which accounts for the EPR Signal II_vf and Signal II_f). The electron carrier responsible for the Z_v band is also a component located prior to the inhibitory site of DCMU (Q⁻_A); its interacting counterpart is an unidentified donor which is involved in charge exchange with the S states.     

Nonlineal relationship between g=2 doublet and multiline signals in Ca(2+)-depleted Photosystem II

Illuminating of the Ca(2+)-depleted PS II in the S(2) state for a short period induced the doublet signal at g=2 with concomitant diminution of the multiline signal, both in the presence and absence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU). In the absence of DCMU, the doublet signal decayed (t(1/2) approximately 7 min) during subsequent dark incubation at 273 K and the multiline signal was regenerated to the original amplitude with the same kinetics of the doublet decay. In the presence of DCMU, the doublet signal decayed much faster (t(1/2) approximately 1 min) by charge recombination with Q(A)(-), while the time course of the multiline recovery was inherently identical with that observed in the absence of DCMU. A simple theoretical consideration indicates the direct conversion from the doublet-signal state to the multiline state with no intermediate state between them. Lengthy dark storage at 77 K led to disappearance of the DCMU-affected doublet signal and a Fe(2+)/Q(A)(-) electron spin resonance (ESR) signal, but no recovery of the multiline signal. Notably, the multiline signal was restored by subsequent dark incubation at 273 K. The charge recombination between Q(A)(-) and the doublet signal species led to a thermoluminescence band at 7 degrees C in a medium at pH 5.5. The peak position shifted to 17 degrees C at pH 7.0, presumably due to a pH-dependent change in the redox property of a donor-side radical species responsible for the doublet signal. Based on these results, redox events in the Ca(2+)-depleted PS II are discussed in contradistinction with the normal processes in oxygen-evolving PS II.     

A demonstration of energy transfer from photosystem II to photosystem I in chloroplasts

Photosystem I activity of Tris-washed chloroplasts was measured at room temperature as the rate of photoreduction of NADP and as the rate of oxygen uptake mediated by methyl viologen in both cases using dichlorophenolindophenol plus ascorbate as the source of electrons for Photosystem I. With both assay systems the rate of electron transport by Photosystem I was stimulated approx. 20 % by the addition of 3-(3,4-dichlorophenyl)-1, 1-dimethylurea which caused the Photosystem II reaction centers to close. Photosystem I activity of chloroplasts was measured at low temperature as the rate of photooxidation of P-700. Chloroplasts suspended in the presence of hydroxylamine and 3-(3,4-dichlorophenyl)-1, 1-dimethylurea were frozen to ?196 °C after adaptation to darkness or after a preillumination at room temperature. The Photosystem II reaction centers of the frozen dark-adapted sample were all open; those of the preilluminated sample were all closed. The rate of photooxidation of P-700 at ?196 °C with the preilluminated sample was approx. 25 % faster than with the dark-adapted sample. We conclude from both the room temperature and the low temperature experiments that there is greater energy transfer from Photosystem II to Photosystem I when the Photosystem II reaction centers are closed and that these results are a direct demonstration of spillover.     

Photooxidation of cytochrome b559 and the electron donors in chloroplast Photosystem II

The effect of light on the reaction center of Photosystem II was studied by differential absorption spectroscopy in spinach chloroplasts.

At − 196 °C, continuous illumination results in a parallel reduction of C-550 and oxidation of cytochrome b₅₅₉ high potential. With flash excitation, C-550 is reduced, but only a small fraction of cytochrome b₅₅₉ is oxidized. The specific effect of flash illumination is suppressed if the chloroplasts are preilluminated by one flash at 0 °C.

At − 50 °C, continuous illumination results in the reduction of C-550 but little oxidation of cytochrome b₅₅₉. However, complete oxidation is obtained if the chloroplasts have been preilluminated by one flash at 0 °C. The effect of preillumination is not observed in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea.

A model is discussed for the reaction center, with two electron donors, cytochrome b₅₅₉ and Z, acting in competition. Their respective efficiency is dependent on temperature and on their states of oxidation. The specific effect of flash excitation is attributed to a two-photon reaction, possibly based on energy-trapping properties of the oxidized trap chlorophyll.     

A differential effect of 3-(3′4′ dichlorophenyl)-1,1 dimethyl urea and atrazine on fluorescence kinetics in chloroplasts

It was found that DCMU had a differential effect at two concentration ranges on variable fluorescence kinetics in isolated chloroplasts. The increase in fluorescence rate at low concentrations of DCMU was abolished by preincubation of chloroplasts with ferricyanide or formate, treatments which were shown to convert Fe in the PS II reaction center (i.e., the FeQ_A complex) into a non-oxidizable form, but it was not affected by Tris treatment. Increase in fluorescence kinetics (at the initial linear rate) at high concentrations of DCMU was found to be abolished by Tris treatment but it was only marginally affected by ferricyanide or formate treatments. The effect of Tris could be abolished by addition of hydroquinone-ascorbate, which restored electron flow to the pool of secondary acceptors.Contrary to the effect of DCMU, no such differential concentration dependence of the variable fluorescence kinetics was found for atrazine.The increase in fluorescence kinetics (at the initial linear rate) at a low concentration rate of DCMU is presumably restricted to units which contain an oxidizable Fe in the FeQ_A complex. Increase in fluorescence kinetics (at the initial linear rate) at high DCMU concentration is probably related to the effect of DCMU at the Q_B site.Abbreviations DCMU 3-(34 dichlorophenyl)-1,1 dimethyl urea - PS II Photosystem II - Tris tris (hydroxymethyl) aminomethane     

Studies on the Component Responsible for the Oxidation of the Primary Electron Acceptor of Photosystem II in the Presence of 3-(3',4'-Dichlorophenyl)-1,1-Dimethyl Urea: Reactivity to External Reductants

The dark reoxidation of the photochemically reduced primaryelectron acceptor of photosystem II, Q., in the presence of3-(3',4'-dichlorophenyl)-l,l-dimethyl urea (DCMU) by the redoxcounterpart (here designated Z) of Q, was studied by monitoringthe dark recovery of the induction of chlorophyll fluorescence. In normal chloroplasts, the dark reoxidation of reduced Q inthe presence of DCMU was not affected by the externally addedhydrophilic reductants; ascorbate, hydroquinone, hydrogen peroxide,manganous chloride, potassium iodide and potassium ferrocyanide.In chloroplasts whose oxidizing side of photosystem II had beeninactivated by heat- or Tris-treatments, reoxidation was inhibitedpartially. This inhibition increased on the addition of hydrophilicreductants, but was relieved by increasing the redox potentialof the suspension medium with the chloroplasts. We concluded that the redox counterpart, Z, of Q, in the presenceof DCMU is located in a hydrophobic environment which can bedenatured by heat- or Tris-treatments to allow the access ofnormally extruded hydrophilic electron donors. (Received January 10, 1981; Accepted March 12, 1981)     

The mechanism of the ozone-induced changes in thermoluminescence glow curves of barley leaves

The changes in thermoluminescence (TL) signals induced by short-term ozone exposure of leaves are characterized by a down-shift of the peak-temperature of the TLB-band and an increase of a TL band at 55°C. We investigated the relationship of these changes to photosystem 2 (PS2) photochemistry. The changes were not only detectable in the presence of ozone, but also after irradiation of dark-adapted leaves and after aging of irradiated detached leaf segments. The opposite effect on TL, an up-shift of the peak-temperature of the B-band and the decrease of the intensity of the band at 55°C were found after infiltration of leaves with nigericin, antimycin A, and diphenyleneiodonium chloride (DPI). Propyl gallate down-shifted the peak-temperature of the B-band. 2,5-dimethyl-1,4-benzoquinone up-shifted the peak-temperature of the B-band and decreased the intensity of the 55°C band. The intensity of the 55°C band did not change significantly in the presence of oxygen in comparison to that in nitrogen atmosphere. It decreased with time of dark adaptation (50% intensity was observed after 3 h of dark adaptation at room temperature), however, it was reactivated to its initial value (at 5 min of dark adaptation) after 1 single-turnover flash. The 55°C band was not significantly changed in the presence of DCMU. Thus the ozone-induced band at 55°C is assigned to charge recombination in PS2. Changes in the electron transport chain at the acceptor side of PS2, probably related to the cyclic electron transport around photosystem 1 and/or chlororespiration, could play an important role in the increase of the 55°C band and the down-shift of the B-band. The changes at the acceptor side indicated by TL can be an ex pression of a physiological regulatory mechanism functional under stress conditions.     

Activation of the non-electrochromic component in the 518 nm absorbance change by photosystem I

The flash-induced absorbance change measured at 518 nm (P515) in intact chloroplasts consists of at least 4 kinetically different components. Here the non-electrochromic component, either called phase d or reaction 3, is studied in some detail. The effect of DCMU, DQH₂ and DBMIB on the amplitude of reaction 3 and the turnover of cytochrome f and P700 have been monitored, suggesting an involvement of photosystem 1 in the activation of the non-electrochromic absorbance change. This is confirmed by the parallel oscillation pattern found in P700 rereduction and the amplitude of reaction 3.     

Thermoluminescence studies on the function of Photosystem II in the desiccation tolerant lichen Cladonia convoluta

The effect of desiccation and rehydration on the function of Photosystem II has been studied in the desiccation tolerant lichen Cladonia convoluta by thermoluminescence. We have shown that in functional fully hydrated thalli thermoluminescence signals can be observed from the recombination of the S₂₍₃₎Q_B ^– (B band), S₂Q_A ^– (Q band), Tyr-D⁺Q_A ^– (C band) and Tyr-Z⁺(His⁺)Q_A ^– (A band) charge stabilization states. These thermoluminescence signals are completely absent in desiccated thalli, but rapidly reappear on rehydration. Flash-induced oscillation in the amplitude of the thermoluminescence band from the S₂₍₃₎Q_B ^– recombination shows the usual pattern with maxima after 2 and 6 flashes when rehydration takes place in light. However, after rehydration in complete darkness, there is no thermoluminescence emission after the 1 st flash, and the maxima of the subsequent oscillation are shifted to the 3rd and 7th flashes. It is concluded that desiccation of Cladonia convoluta converts PS II into a nonfunctional state. This state is characterized by the lack of stable charge separation and recombination, as well as by a one-electron reduction of the water-oxidizing complex. Restoration of PS II function during rehydration can proceed both in the light and in darkness. After rehydration in the dark, the first charge separation act is utilized in restoring the usual oxidation state of the water-oxidizing comples.Abbreviations Chl chlorophyll - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - DT desiccation tolerant - PS II Photosystem II - TL thermoluminescence - P₆₈₀ reaction center Chl of PS II - Q_A and Q_B puinone electron acceptors of PS II - S₀,...,S₄ the redox states of the water-oxidizing complex - Tyr-Z and Tyr-D redox-active tyrosine electron donors of PS II     

Lipid biosynthesis by isolated plastids from greening pea, Pisum sativum

Isolated etioplasts from 8-day-old dark-grown pea seedlings incorporated [1-(14)C]acetate into lipid at a relatively low rate. Plastids from seedlings that had been illuminated for at least 2 hr showed an enhanced incorporation provided the plastids were illuminated during incubation with the labeled acetate. Dark incubation or the addition of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) decreased the acetate-incorporating activity of the developing chloroplasts to the level observed with etioplasts. Light had a marked effect on the type of fatty acid into which acetate was incorporated by the developing chloroplasts. Unsaturated fatty acids (mostly oleic acid) accounted for 60-80% of the incorporated label if the plastids were illuminated, but in the dark or in the presence of DCMU the unsaturated acids accounted for only 0-15% of the label incorporated into lipid. The effect of ATP on incorporation was dependent on the maturity of the chloroplasts; mature pea chloroplasts were inhibited by ATP, whereas in developing plastids there was a slight stimulation by ATP. Inhibition of acetate incorporation into lipid by DCMU appears to be due to inhibition of noncyclic phosphorylation. Incorporation was restored by reduced 2,3,5,6-tetramethylphenylenediamine, which restored phosphorylation, but not by reduced N,N,N',N'-tetramethylphenylenediamine.     

Chlorophyll radical cation in photosystem II of chloroplasts. Millisecond decay at low temperature.

We compare the absorption changes, in the near infrared and in the green part of the spectrum, induced in spinach chloroplasts suspensions, at -- 170 degrees C, by continuous light and by flashes. (1) Following flash excitation, an absorption increase peaking at 825 nm which reverses rapidly (t 1/2 = 3.0 ms) is not affected by ferricyanide; it is suppressed when chloroplasts are preilluminated in the presence of 3-(3',4'-dichlorophenyl)-1,1'-dimethylurea (DCMU) and hydroxylamine. The reversion of that signal is simultaneous with a partial back reoxidation of C-550 (fully reduced by the flash) and with partial (about 25%) oxidation of cytochrome b559. The magnitude of the signal peaking at 825 nm (that we attribute to the radical cation of the trap chlorophyll of Photosystem II, acting as a primary electron donor) decreases progressively within a series of successive flashes. (2) An absorption increase (40% of which is slowly reversible) with a broad peak around 810 nm is induced by continuous light or by a flash. It is suppressed by pretreatment with ferricyanide, but it is little affected by the treatment with 3-(3',4'-dichlorophenyl)-1,1'-dimethylurea and hydroxylamine. We attribute it to oxidized P700. (3) With chloroplasts pretreated with 10 mM ferricyanide, an absorption increase, whose magnitude is nearly independent of wavelength between 790 and 870 nm, can be induced by continuous light. One saturating flash produces only 20% of the signal. This absorption change (20% of which is reversible in 30 s) might be due to a secondary donor of Photosystem II.     

Heterogeneity of system II secondary electron acceptors in Tris-washed chloroplasts

Tris-washed chloroplasts were submitted to saturating short flashes, and then rapidly mixed with dichlorophenyldimethylurea (DCMU). The amount of singly reduced secondary acceptor was estimated from the DCMU-induced increase in fluorescence, caused by the reverse electron flow from secondary to primary acceptor. The back-transfer from the singly reduced secondary acceptor to the primary acceptor Q induced by DCMU addition affects only a part (60%) of the variable fluorescence (ΔF_max). As previously shown, the quenchers involved in this phenomenon, ‘B-type’ quenchers, are different from those controlling the complementary part of the fluorescence, the non-B-type. In this report, we show that at pH 8.5 in the B-type systems, there exist two kinds of secondary electron acceptors: B, a two-electron acceptor, the corresponding Q accounting for 40% of the variable fluorescence; B′, a one-electron acceptor, the corresponding Q accounting for 20% of the variable fluorescence. The lifetimes of B^? and B′^? in the absence of DCMU are 40 and 1 s, respectively. The primary acceptors of the B and B′ systems can be considered as corresponding to the Q₁s defined previously (Joliot, P. and Joliot, A. (1981) in Proceedings of the 5th International Congress on Photosynthesis (Akoynoglou, G., ed.), pp. 885–899, Balaban International Science Services, Philadelphia). The B′ centers seems to be equivalent to the Q_β centers as defined by other workers (Van Gorkom, H.J., Thielen, A.P.G.M. and Gorren, A.C.F. (1982) in The Function of Quinones in Energy Conserving Systems (Trumpower, B.L., ed.), Academic Press, New York, in the press).