Regulation of Photosystem Stoichiometry in the Photosynthetic System of the Cyanophyte Synechocystis PCC 6714 in Response to Light-Intensity

Light-induced changes in stoichiometry among three thylakoidcomponents, PS I, PS II and Cyt b₆-f complexes, were studiedwith the cyanophyte Synechocystis PCC 6714. Special attentionwas paid to two aspects of the stoichiometric change; first,a comparison of the patterns of regulation in response to differencesin light-intensity with those induced by differences in light-quality,and second, the relationship between regulation of the stoichiometryand the steady state of the electron transport system. Resultsfor the former indicated that (1) the abundance of PS I on aper cell basis was reduced under white light at the intensityas high as that for light-saturation of photosynthesis, butPS I per cell was increased under low light-intensity, (2) PSII and Cyt b₆-f complexes remained fairly constant, and (3)changes in the abundance of PS I depended strictly on proteinsynthesis. The pattern was identical with that of chromaticregulation. For the second problem, the redox steady-statesof Cyt f and P700 under white light of various intensities weredetermined by flash-spectroscopy. Results indicated that (1)Cyt f and P700 in cells grown under low light-intensity [highratio of PS I to PS II (PS I/PS II)] were markedly oxidizedwhen the cells were exposed to high light-intensity, while theyremained in the reduced state under low light-intensity. (2)After a decrease in the abundance of PS I, most of P700 remainedin the reduced state even under high light-intensity, whilethe level of reduced Cyt f remained low. (3) Both Cyt f andP700 in cells of low PS I/PS II were fully reduced under lowlight-intensity, and Cyt f reduction following the flash wasrapid, which indicates that the turnover of PS I limits theoverall rate of electron flow. After an increase in the abundanceof PS I, the electron transport recovered from the biased state.(4) The redox steady-state of the Cyt b₆-f complex correlatedwell with the regulation of PS I/PS II while the state of thePQ pool did not. Based on these results, a working model ofthe regulation of assembly of the PS I complex, in which theredox steady-state of the Cyt b₆-f complex is closely relatedto the primary signal, is proposed. (Received August 2, 1990; Accepted December 10, 1990)     

Regulation of Electron Transport Composition in Cyanobacterial Photosynthetic System: Stoichiometry among Photosystem I and II Complexes and Their Light-Harvesting Antennae and Cytochrome b6/fComplex

This study was done to confirm our previous observation withthe pattern of changes in electron transport composition inducedby an imbalance of the electron transport state. Contents ofphotosystem (PS) I and II complexes and their antennae and Cytb₆/f complex were determined for systems of cyanobacterium SynechocystisPCC 6714 of different PS I/PS II ratios. The results indicatedthat (1) the observed changes in the PS I/PS II ratio are not-dueto regulation of the activities of the respective PS's but tochanges in their contents, (2) the molar ratio between PS IIand Cyt b₆/f complexes was fairly constant when marked changesoccurred in the PS I content, and (3) the PS II and Cyt b₆/fcontents per cell remained fairly constant while the PS I contentchanged markedly. These findings agree with our previous observationwith autotrophic cells of Anacystis nidulans Tx 20 and supportour argument that in cyanobacterial and red algal electron transportsystems, the content of the terminalcomponent(s), such as PSI complex, is regulated in order to maintain a balance betweenthe electron influx by PS II action to the system and the effluxby PS I action from it. (Received June 3, 1987; Accepted September 20, 1987)     

Effect of Supra-High Irradiation on the Photosynthetic System of the Cyanophyte Synechocystis PCC 6714

Stability of thylakoid components under supra-high irradiancewas studied with the cyanophyte Synechocystis PCC 6714. Theactivity of overall photosynthesis was quickly inactivated (T_1/2=20min) under supra-high irradiance (300 W m^–2, white light).In parallel with the inactivation of photosynthesis, QA in PSII was also inactivated. Both inactivations were acceleratedby chloramphenicol (CAP) addition. The reactivation of PS IIrequired weak irradiation and was suppressed by CAP. However,PS I measured as P700 was very stable. The level of PS I measuredas P700 was not significantly reduced by the irradiation for12 h even in the presence of CAP while the level of Cyt b₅₅₉,component of PS II, was decreased markedly. The function ofPS I before and after supra-high irradiation with CAP was examinedby comparing sizes of P700 oxidation induced by a short flash,by a continuous light, and by determination of O₂-and ferredoxin-reduction.No difference was observed in PS I actions before and afterthe irradiation treatment. These results indicate that the PSI complex is very tolerant of supra-high irradiation. However,the cells grown under supra-high irradiance contained much fewerPS I and PS II complexes than Cyt b₆–f complexes. Theformer levels were reduced to a half to one fourth of thosebefore growth while the level of Cyt b₆–f complex wasnot reduced so much. A possible mechanism for changes in thylakoidcomposition under supra-high irradiation was discussed. (Received February 16, 1991; Accepted June 12, 1991)     

Quantitative analysis of 77K fluorescence emission spectra in Synechocystis sp. PCC 6714 and Chlamydomonas reinhardtii with variable PS I/PS II stoichiometries

Low-temperature (77 K) fluorescence emission spectra of intact cells of a cyanobacterium, Synechocystis sp. PCC 6714, and a green alga, Chlamydomonas reinhardtii, were quantitatively analyzed to examine differences in PS I/PS II stoichiometries. Cells cultured under different spectral conditions had various PS I/PS II molar ratios when estimated by oxidation-reduction difference absorption spectra of P700 (for PS I) and Cyt b-559 (for PS II) with thylakoid membranes. The fluorescence emission spectra under the Chl a excitation at 435 nm were resolved into several component bands using curve-fitting methods and the relative band area between PS II (F685 and F695) and PS I (F710 or F720) emissions was compared with the PS I/PS II stoichiometries of the various cell types. The results indicated that the PS I/PS II fluorescence ratios correlated closely with photosystem stoichiometries both in Synechocystis sp. PCC 6714 and in C. reinhardtii grown under different light regimes. Furthermore, the correlation between the PS I/PS II fluorescence ratios and the photosystem stoichiometries is also applicable to vascular plants.     

Light-induced Changes of the Electrical Potential in Chloroplasts Associated with the Activity of Photosystem I and Photosystem II

The electric potential changes induced by flashing and continuouslight were measured with microcapillary electrodes in isolatedwhole chloroplasts of Peperomia inetallica. In continuous lightthe chloroplast electrical potential rose in two phases. Theinitial rapid phase coincided in extent with the flash-inducedpotential and was insensitive to the electron transfer inhibitorDBMIB. The subsequent phase was relatively slow (20–30ms) and was inhibited by DBMIB. Electron acceptors of photosystemII (p-phenylendiamine, p-benzoquinone) added to DBMIB-treatedchloroplasts produced a suppression of the flash-induced responseand a considerable increase in the steady level of the potentialin the light. The electrical potential associated with the activityof photosystem II rose in continuous light much more slowlythan that associated with the activity of photosystem I aloneor the activities of both photosystems. Illumination of chloroplastswith successive flashes at a repetition rate 5 Hz in the presenceof oxaloacetate, a terminal acceptor of photosystem I, was accompaniedwith a gradual decline of the flash-induced potential. The specificrole of two photosystems in the light-induced H⁺ transport andthe electrogenesis across the chloroplast thylakoid membranesis discussed.     

Regulation of Stoichiometry between PSI and PSII in Response to Light Regime for Photosynthesis Observed with Synechocystis PCC 6714: Relationship between Redox State of Cyt b6-f Complex and Regulation of PSI Formation

The effect of the Cyt b₆-f redox state on the PSI formationwas examined with the cyanophyte Synechocystis PCC 6714 by usinga Q-cycle inhibitor, HQNO (2-n-heptyl-4-hydroxyquinoline N-oxide).HQNO inhibited the rapid reduction of flash-oxidized Cyt f,the reaction correlating with the stimulation of PSI formation,on one hand, and accumulated reduced Cyt b₆, on the other, indicatingthat the electron flow in the Q-cycle correlates with regulationof PSI synthesis. HQNO also inhibited the stimulation of PSIformation under PSII light, resulting in a low PSI/PSII ratioeven under PSII light, while the PSI formation under PSI lightwas not suppressed by HQNO. Simultaneous inhibition of Cyt b₆oxidation through the Q-cycle and the stimulated PSI formationby HQNO suggests that an HQNO-sensitive Cyt b₆ oxidation isinvolved in the mechanism of monitoring the state of electrontransport system for regulation of PSI formation. (Received March 3, 1993; Accepted August 9, 1993)     

Steady State of Photosynthesis in Cyanobacterial Photosynthetic Systems Before and After Regulation of Electron Transport Composition: Overall Rate of Photosynthesis and PSI/PS II Composition

The effect of regulation of photosystem (PS) composition onthe photosynthetic steady state was examined using the cyanobacteriumSynechocystis PCC 6714. Photosynthetic rates under orange lightabsorbed by phycobiliprotein (PBP) (PBP light) and under redlight absorbed mainly by chlorophyll a (Chi a light) were comparedfor the cells before and after adaptation to the respectivelight regimes. Results were as follows: (1) Photosynthetic ratesper absorbed light quantum became higher after adaptation thanthose before adaptation. (2) Under Chi a light, the low turnoverrate of PS I before adaptation was markedly enhanced after adaptation(decrease in PS I content), but in the case of adaptation toPBP light (increase in PS I content), a marked enhancement ofPS II turnover occurred after adaptation. (3) In the formercase, a low turnover rate of PS I before adaptation was dueto the occurrence of a large number of closed PS I complexes,but in the latter, limited excitation of PS I caused a largenumber of closed PS II complexes before adaptation. Resultsfor the latter case indicate that the energy transfer from phycobilisome(PBS) to one PS I complex is far smaller than that from PBSto one PS II complex, and that the imbalance of energy distributionfrom PBS to the two photosystems is compensated for by the increasein the number of PS I complexes. (Received September 10, 1987; Accepted December 9, 1987)     

Photosynthetic Electron Transport During Senescence of the Primary Leaves of Phaseolus vulgaris L.: II. THE ACTIVITY OF PHOTOSYSTEMS ONE AND TWO, AND A NOTE ON THE SITE OF REDUCTION OF FERRICYANIDE

The activity of photosystems one and two (PS I and PS II) wasmeasured in chloroplasts isolated from the primary leaves ofPhaseolus vulgaris. During foliar senescence, the rates of electrontransport through PS I and PS II declined by approximately 25%and 33% respectively. These losses of activity could not accountfor the decrease of 80% in the rate of coupled, non-cyclic electrontransport during senescence. It is therefore suggested thatan impairment of electron flow between the photosystems limitednon-cyclic electron transport in chloroplasts from older leaves.In this study the activity of PS II was measured using oxidizedp-phenylenediamine as the electron acceptor, and trifluralinas an inhibitor of electron transport between PS II and PS I.In chloroplasts from young leaves the reduction of ferricyanidewas a measure of non-cyclic electron transport, but in preparationsfrom older leaves ferricyanide received a large proportion ofelectrons from PS II.     

Determination of the PS I content of PS II core preparations using selective emission: A new emission of PS II at 780 nm

Routinely prepared PS II core samples are often contaminated by a significant (~ 1–5%) fraction of PS I, as well as related proteins. This contamination is of little importance in many experiments, but masks the optical behaviour of the deep red state in PS II, which absorbs in the same spectral range (700–730 nm) as PS I (Hughes et al. 2006). When contamination levels are less than ~ 1%, it becomes difficult to quantify the PS I related components by gel-based, chromatographic, circular dichroism or EPR techniques. We have developed a fluorescence-based technique, taking advantage of the distinctively different low-temperature emission characteristics of PS II and PS I when excited near 700 nm. The approach has the advantage of providing the relative concentration of the two photosystems in a single spectral measurement. A sensitivity limit of 0.01% PS I (or better) can be achieved. The procedure is applied to PS II core preparations from spinach and Thermosynechococcus vulcanus. Measurements made of T. vulcanus PS II preparations prepared by re-dissolving crystallised material indicate a low but measurable PS I related content. The analysis provides strong evidence for a previously unreported fluorescence of PS II cores peaking near 780 nm. The excitation dependence of this emission as well as its appearance in both low PS I cyanobacterial and plant based PS II core preparations suggests its association with the deep red state of PS II.     

Mechanism of the light state transition in photosynthesis. I. Analysis of the kinetics of cytochrome f oxidation in State 1 and State 2 in the red alga, Porphyridium cruentum

The kinetics of photooxidation and reduction of cytochrome f were examined spectrophotometrically in the red alga Porphyridium cruentum in light State 1 and light State 2. Experiments were performed on intact cells that had been chemically fixed and stabilized in the light states. The cytochrome f turnover was measured during conditions of linear electron transport driven by both photosystems and during several cyclic reactions mediated by the long-wavelength Photosystem (PS) I. The data show that the rate of photooxidation of cytochrome f increased in State 2 when the cells were activated by subsaturating intensities of green light absorbed primarily by the phycobilisome. No differences in kinetics were found between algae in State 1 or State 2 when they were activated by light absorbed primarily by the chlorophyll of PS I. The results confirm that changes in energy distribution between the two photosystems occur as a result of the light state transition and verify that the redistribution of excitation results in the predicted changes in electron transport.     

Action Spectra of Photosystems I and II in State 1 and State 2 in Intact Sugar Maple Leaves

Photochemical activity, measured as energy storage of photosystems I (PSI) and II (PSII) together and individually, is studied in sugar maple (Acer saccharum Marsh.) leaves in the spectral range between 400 and 700 nm in state 1 and state 2. Total photochemical activity remains the same in both state 1 and state 2 between 580 and 700 nm, but it is lower in state 2 between 400 and 580 nm. Both PSI and PSII activities change significantly during the state transition due to the migration of light-harvesting chlorophyll a/b protein complex of PSII (LHCII). In the action spectra of PSI and PSII, peak positions vary depending on the association or dissociation of LHCII, except for the peak at 470 nm in the PSII spectrum. PSII activity is about 3 times higher than or equal to PSI in state 1 or state 2, respectively, over most of the spectrum except in the blue and far-red regions. At 470 nm, PSII activity is 8 or 1.6 times higher than PSI in state 1 or state 2, respectively. The amplitude of LHCII coupling-induced change is the same in both PSI and PSII between 580 and 700 nm, but it is less in PSI than in PSII between 400 and 580 nm, which explains the lower photochemical activity of the leaf in state 2 than in state 1. This may be due to a decrease in energy transfer efficiency of carotenoids to chlorophylls in LHCII when it is associated with PSI.     

Chromatic Regulation in Chlamydomonas reinhardtii: Time Course of Photosystem Stoichiometry Adjustment Following a Shift in Growth Light Quality

Photosystem stoichiometry adjustments in Chlamydomonas reinhardtiiwere induced upon a sudden shift in the light quality duringcell growth. Reversible changes in the PSI/PSII ratio were acompensation response to changes in the balance of light absorptionby the two photosystems. Quantitations of PSII, Cyt b₆-f complexand PSI revealed a constancy in the cellular content of PSIIand the Cyt b₆-f complex, and variable amounts of PSI in C.reinhardtii. These results strengthen the notion that PSI isthe thyla-koid component subject to chromatic regulation andresponsible for the adjustment and optimization of the PSI/PSII ratio in the thylakoid of oxygenic photosynthesis. Additionalresults, obtained upon the use of protein biosynthesis translationinhibitors (chloramphenicol and cyclohex-imide), suggested thata chromatically-induced lowering of the PSI/PSII ratio in C.reinhardtii occurs by suppression of de novo biosynthesis ofPSI components and, therefore, by dilution of the PSI complexin the thylakoid membrane, rather than by active degradationof assembled PSI in chlo-roplasts. (Received November 8, 1996; Accepted December 6, 1996)     

Investigation of the apparent inefficiency of the coupling between Photosystem II electron transfer and ATP formation

The maximum phosphorylation efficiency achieved with synchronous turnovers of Photosystem II (PS II) in spinach chloroplast lamellae is 0.3 molecules of ATP per pair of electrons transferred. This is the same as the efficiency observed for PS II operating alone in continuous light and would seem to indicate less than 50% coupling efficiency. Flash-induced ATP synthesis associated with both photosystems acting in unison closely approaches twice the flash-induced ATP synthesis associated with the Photosystem-I-dependent oxidation of duroquinol (itself 0.6) and comes close to equalling the highest efficiency observed in steady-state PS I + PS II electron transport. The anomalously low coupling efficiency seen when PS II is operating alone can be overcome by a ΔpH of two units imposed before flash illumination, or by a prior flash series involving the entire electron transfer chain. In contrast, prior electron transport through PS II alone is only slightly effective in enhancing the coupling efficiency of subsequent PS II turnovers. (It should be noted that in all cases where supplementary energy was provided, either by a proton gradient or by prior illumination, this supplementary energy was always below the energetic threshold for phosphorylation. Furthermore, the enhancement of PS II coupling efficiency by supplementary energy persisted even after a large number of subsequent PS II-inducing flashes). The efficiency of flash-induced ATP synthesis associated with whole-chain electron transfer or with PS-I-dependent duroquinol oxidation is also enhanced by the supplementary energy, but only during the first few inefficient flashes, suggesting that in this case the supplementary energy may simply be contributing to the initial build-up of an energetic threshold for ATP synthesis. This cannot be the case when the same supplementary energy contributes to the efficiency of the PS II reaction, since the enhancement then persists for a long time and contributes to an essentially constant flash yield of ATP. Our results imply that during electron transfer involving both photosystems, PS II participates in generating about half of the total ATP, whereas it operates inefficiently only when operating alone. Since hydrogen ions produced by PS I are able to raise the efficiency of subsequent PS-II-dependent phosphorylation, at least some cooperation between the two photosystems takes place and this suggests some donation of protons from PS I to PS II. However, the inability of PS II alone to achieve high efficiency, even with prolonged pre-illumination, would seem to indicate some functional distinction of protons from the two photosystems.     

Deciphering the 820 nm signal: redox state of donor side and quantum yield of Photosystem I in leaves

By recording leaf transmittance at 820 nm and quantifying the photon flux density of far red light (FRL) absorbed by long-wavelength chlorophylls of Photosystem I (PS I), the oxidation kinetics of electron carriers on the PS I donor side was mathematically analyzed in sunflower (Helianthus annuus L.), tobacco (Nicotiana tabacum L.) and birch (Betula pendula Roth.) leaves. PS I donor side carriers were first oxidized under FRL, electrons were then allowed to accumulate on the PS I donor side during dark intervals of increasing length. After each dark interval the electrons were removed (titrated) by FRL. The kinetics of the 820 nm signal during the oxidation of the PS I donor side was modeled assuming redox equilibrium among the PS I donor pigment (P700), plastocyanin (PC), and cytochrome f plus Rieske FeS (Cyt f + FeS) pools, considering that the 820 nm signal originates from P700⁺ and PC⁺. The analysis yielded the pool sizes of P700, PC and (Cyt f + FeS) and associated redox equilibrium constants. PS I density varied between 0.6 and 1.4 μmol m⁻². PS II density (measured as O₂ evolution from a saturating single-turnover flash) ranged from 0.64 to 2.14 μmol m⁻². The average electron storage capacity was 1.96 (range 1.25 to 2.4) and 1.16 (range 0.6 to 1.7) for PC and (Cyt f + FeS), respectively, per P700. The best-fit electrochemical midpoint potential differences were 80 mV for the P700/PC and 25 mV for the PC/Cyt f equilibria at 22 °C. An algorithm relating the measured 820 nm signal to the redox states of individual PS I donor side electron carriers in leaves is presented. Applying this algorithm to the analysis of steady-state light response curves of net CO₂ fixation rate and 820 nm signal shows that the quantum yield of PS I decreases by about half due to acceptor side reduction at limiting light intensities before the donor side becomes oxidized at saturating intensities. Footnote: This revised version was published online in August 2006 with corrections to the Cover Date.     

Control of cytochrome b6f at low and high light intensity and cyclic electron transport in leaves

The light-dependent control of photosynthetic electron transport from plastoquinol (PQH(2)) through the cytochrome b(6)f complex (Cyt b(6)f) to plastocyanin (PC) and P700 (the donor pigment of Photosystem I, PSI) was investigated in laboratory-grown Helianthus annuus L., Nicotiana tabaccum L., and naturally-grown Solidago virgaurea L., Betula pendula Roth, and Tilia cordata P. Mill. leaves. Steady-state illumination was interrupted (light-dark transient) or a high-intensity 10 ms light pulse was applied to reduce PQ and oxidise PC and P700 (pulse-dark transient) and the following re-reduction of P700(+) and PC(+) was recorded as leaf transmission measured differentially at 810-950 nm. The signal was deconvoluted into PC(+) and P700(+) components by oxidative (far-red) titration (V. Oja et al., Photosynth. Res. 78 (2003) 1-15) and the PSI density was determined by reductive titration using single-turnover flashes (V. Oja et al., Biochim. Biophys. Acta 1658 (2004) 225-234). These innovations allowed the definition of the full light response curves of electron transport rate through Cyt b(6)f to the PSI donors. A significant down-regulation of Cyt b(6)f maximum turnover rate was discovered at low light intensities, which relaxed at medium light intensities, and strengthened again at saturating irradiances. We explain the low-light regulation of Cyt b(6)f in terms of inactivation of carbon reduction cycle enzymes which increases flux resistance. Cyclic electron transport around PSI was measured as the difference between PSI electron transport (determined from the light-dark transient) and PSII electron transport determined from chlorophyll fluorescence. Cyclic e(-) transport was not detected at limiting light intensities. At saturating light the cyclic electron transport was present in some, but not all, leaves. We explain variations in the magnitude of cyclic electron flow around PSI as resulting from the variable rate of non-photosynthetic ATP-consuming processes in the chloroplast, not as a principle process that corrects imbalances in ATP/NADPH stoichiometry during photosynthesis.     

The stoichiometry and antenna size of the two photosystems in marine green algae, Bryopsis maxima and Ulva pertusa, in relation to the light environment of their natural habitat

The stoichiometry and antenna sizes of the two photosystems in two marine green algae, Bryopsis maxima and Ulva pertusa, were investigated to examine whether the photosynthetic apparatus of the algae can be related to the light environment of their natural habitat. Bryopsis maxima and Ulva pertusa had chlorophyll (Chl) a/b ratios of 1.5 and 1.8, respectively, indicating large levels of Chl b, which absorbs blue-green light, relative to Chl a. The level of photosystem (PS) II was equivalent to that of PS I in Bryopsis maxima but lower than that of PS I in Ulva pertusa. Analysis of Q(A) photoreduction and P-700 photo-oxidation with green light revealed that >50% of PS II centres are non-functional in electron transport. Thus, the ratio of the functional PS II to PS I is only 0.46 in Bryopsis maxima and 0.35 in Ulva pertusa. Light-response curves of electron transport also provided evidence that PS I had a larger light-harvesting capacity than did the functional PS II. Thus, there was a large imbalance in the light absorption between the two photosystems, with PS I showing a larger total light-harvesting capacity than PS II. Furthermore, as judged from the measurements of low temperature fluorescence spectra, the light energy absorbed by Chl b was efficiently transferred to PS I in both algae. Based on the above results, it is hypothesized that marine green algae require a higher ATP:NADPH ratio than do terrestrial plants to grow and survive under a coastal environment.     

Control of cytochrome b6f at low and high light intensity and cyclic electron transport in leaves

The light-dependent control of photosynthetic electron transport from plastoquinol (PQH₂) through the cytochrome b₆f complex (Cyt b₆f) to plastocyanin (PC) and P700 (the donor pigment of Photosystem I, PSI) was investigated in laboratory-grown Helianthus annuus L., Nicotiana tabaccum L., and naturally-grown Solidago virgaurea L., Betula pendula Roth, and Tilia cordata P. Mill. leaves. Steady-state illumination was interrupted (light-dark transient) or a high-intensity 10 ms light pulse was applied to reduce PQ and oxidise PC and P700 (pulse-dark transient) and the following re-reduction of P700⁺ and PC⁺ was recorded as leaf transmission measured differentially at 810-950 nm. The signal was deconvoluted into PC⁺ and P700⁺ components by oxidative (far-red) titration (V. Oja et al., Photosynth. Res. 78 (2003) 1-15) and the PSI density was determined by reductive titration using single-turnover flashes (V. Oja et al., Biochim. Biophys. Acta 1658 (2004) 225-234). These innovations allowed the definition of the full light response curves of electron transport rate through Cyt b₆f to the PSI donors. A significant down-regulation of Cyt b₆f maximum turnover rate was discovered at low light intensities, which relaxed at medium light intensities, and strengthened again at saturating irradiances. We explain the low-light regulation of Cyt b₆f in terms of inactivation of carbon reduction cycle enzymes which increases flux resistance. Cyclic electron transport around PSI was measured as the difference between PSI electron transport (determined from the light-dark transient) and PSII electron transport determined from chlorophyll fluorescence. Cyclic e⁻ transport was not detected at limiting light intensities. At saturating light the cyclic electron transport was present in some, but not all, leaves. We explain variations in the magnitude of cyclic electron flow around PSI as resulting from the variable rate of non-photosynthetic ATP-consuming processes in the chloroplast, not as a principle process that corrects imbalances in ATP/NADPH stoichiometry during photosynthesis.     

Coregulation of electron transport through PS I by Cyt b 6 f,excitation capture by P700 and acceptor side reduction. Time kinetics and electron transport requirement

Regulation of electron transport rate through Photosystem I (PS I) was investigated in intact sunflower leaves. The rate constant of electron donation via the cytochrome b ₆ f complex (k_q, s^–1) was obtained from the postillumination P700⁺ reduction rate, measured as the exponential decay of the light-dark difference (D830) of the 830 nm transmission signal. D830 corresponding to maximum oxidisable P700 (D830_m) was obtained by applying white light flashes of different intensity and extrapolating the plot of the quantum yield Y vs. D830 to the axis of abscissae (Y->0). Maximum quantum yield of PS I at completely reduced P700 (Y_m) was obtained by extrapolating the same plot to the axis of ordinates (D830->0). Regulation of k_q, D830_m and Y_m under rate-limiting CO₂ and O₂ concentrations applied after air (21% O₂, 310 ppm CO₂) was investigated. The amplitude of the downregulation of k_q (photosynthetic control) was maximal when electron transport rate (ETR) was limited to about 3 nmol cm^–2 s^–1 and decreased when ETR was higher or lower. Downregulation did not occur in the absence of CO₂ and O₂. These gases acted only as substrates of ribulosebisphosphate carboxylase-oxygenase, no high-affinity reaction of O₂ leading to enhanced photosynthetic control (e.g. Mehler reaction) was detected. After the transition, D830_m at first decreased and then increased again, showing that the reduction of the PS I acceptor side disappeared as a result of the downregulation of k_q. The variation of Y_m had two reasons, PS I acceptor side reduction and variable excitation capture efficiency by P700. It is concluded that electron transport through PS I is coregulated by the rate of plastoquinol oxidation at Cyt b ₆ f, excitation capture efficiency by P700, and by acceptor side reduction.Abbreviations Cyt b ₆ f cytochrome b ₆ f complex - D830 difference of the 830 nm signal from the dark level - ETR electron transport rate - PAD photon absorption density nmol cm^–2 s^–1 - PFD incident photon flux density, nmol cm^–2 s^–1 - PS I Photosystem I - PS II Photosystem II - PQH₂ plastoquinol - P700 Photosystem I donor pigment - Y quantum yield of PS I electron transport, rel. un.     

Identification and characterization of Arabidopsis mutants with reduced quenching of chlorophyll fluorescence

Regulation of nonradiative dissipation of absorbed light energy in PSII is an indispensable process to avoid photoinhibition in plants. To dissect molecular mechanisms of the regulation, we identified Arabidopsis mutants with reduced quenching of Chl fluorescence using a fluorescence imaging system. By analyses of Chl fluorescence induction pattern in the light and quantum yield of both photosystems, 37 mutants were classified into three groups. The first group was characterized by an extremely high level of minimum Chl fluorescence at the open PSII center possibly due to a defect in PSII. Mutants with significant reduction in the nonphotochemical quenching formation but not in quantum yield of both photosystems were classified into the second group. Mutants in the third group showed reduction in quantum yield of both photosystems possibly due to a defect in the electron transport activity. Mutants in the second and third groups were further characterized by light intensity dependence of Chl fluorescence parameters and steady state redox level of P700.     

Control of the Quantum Efficiencies of Photosystems I and II, Electron Flow, and Enzyme Activation following Dark-to-Light Transitions in Pea Leaves: Relationship between NADP/NADPH Ratios and NADP-Malate Dehydrogenase Activation State

The quantum efficiencies of photosystems I and II (PSI and PSII), [NADP]/[NADPH] ratios, and the activities of chloroplastic fructose-1,6-bisphosphatase and NADP-malate dehydrogenase were measured in intact pea (Pisum sativum L.) leaves in air following the transition from darkness to 750 microeinsteins per square meter per second irradiance. PSII efficiency declined from a low value to a minimum within the first 10 to 15 seconds of irradiance, after which it increased progressively to the steady-state value. The resistance of electron flow between the photosystems was high at this time, but it was not the principal factor limiting electron flow. Oxidation of P700 was restricted by acceptor side processes for approximately the first 60 seconds of illumination. Once the acceptor side limitation was relieved, the oxidation state of P700 was used to estimate the quantum efficiency of electron transport by PSI. This was observed to increase progressively with time. The quantum efficiencies of both photosystems increased in parallel, consistent with a predominant role for noncyclic electron transport. Fructose-1,6-bisphosphatase activity increased in an approximately sigmoidal fashion with time of irradiance, paralleling the changes in the quantum efficiencies of the photosystems. In contrast, the activation of NADP-malate dehydrogenase did not show a lag period but increased with time, reaching a maximum value at about 50 seconds of illumination, after which it declined. The NADP pool was not extensively reduced during the first 10 seconds of illumination, but became so subsequently. It remained in the reduced state until about 60 seconds of illumination and then became relatively oxidized. The empirical relationship between NADP-malate dehydrogenase activity and the reduction state of the NADP pool supports the suggestion that NADP-malate dehydrogenase activity is a useful estimate of the reduction state of the stroma.