Electron-transfer reactions in manganese-depleted photosystem II

We have used flash-detection optical and electron paramagnetic resonance spectroscopy to measure the kinetics and yield per flash of the photooxidation of cytochrome b559 and the yield per flash of the photooxidation of the tyrosine residue YD in Mn-depleted photosystem II (PSII) membranes at room temperature. The initial charge separation forms YZ+ QA-. Following this, cytochrome b559 is oxidized on a time scale of the same order and with the same pH dependence as is observed for the decay of YZ+; under the conditions of our experiments, the decay of YZ+ is determined by the lifetime of YZ+ QA-. In order to explain this observation, we have constructed a model for electron donation in which YZ+ and P680+ are in redox equilibrium and cytochrome b559 and YD are oxidized via P680+. Using our results, together with data from earlier investigations of the kinetics of electron transfer from YZ to P680+ and charge recombination of YZ+ QA-, we have obtained the first global fit for electron donation in Mn-depleted PSII that accounts for the data over the pH range from 5 to 7.5. From these calculations, we have obtained the intrinsic rate constants of all the electron-donation reactions in Mn-depleted PSII. These rate constants allow us to calculate the free energy difference between YZ+ P680 and YZ P680+, which is found to increase by 47 +/- 4 mV/pH from pH 5 to 6 and is observed to increase more slowly per pH unit for pH greater than 6. An important conclusion of our experimental work is that the rates of photooxidation of cytochrome b559 and YD are determined by the lifetime of the oxidizing equivalent on YZ/P680. Extension of our model to oxygen-evolving PSII samples leads to the prediction that the kinetics and yields of electron donation from cytochrome b559 and YD to P680+ will depend on the S2- or S3-state lifetime.     

A possible role of redox-active histidine in the photoligation of manganese into a photosynthetic O2-evolving enzyme.

Our previous experiments with a histidine modifier suggest that in Mn-depleted photosystem (PS) II a histidine residue is photooxidized and charge recombination between the oxidized histidine and QA-emits the thermoluminescence AT-band [Ono, T., & Inoue, Y. (1991) FEBS Lett. 278, 183-186]. By use of the AT-band as an index for histidine oxidation, and EPR signals IIf and IIs as indexes for tyrosine oxidation, we studied the role of this putative redox-active histidine in the photoactivation of the O2-evolving enzyme in NH2OH-treated PSII. The following results have been obtained. (i) Strong-light photoinhibition of NH2OH-treated PSII quickly impaired both capabilities of photoactivation and AT-band emission with almost the same half-inhibition time of 1-2 s, while signal IIf was well retained and signal IIs was not affected at all after complete loss of photoactivation capability. (ii) The capability of exogenous Mn2+ photooxidation was relatively sensitive to strong-light photoinhibition, but DPC was relatively sensitive to strong-light photoinhibition, but DPC photooxidation was highly resistant. (iii) Weak-light photoinhibition simultaneously impaired the capabilities of photoactivation, AT-band emission, and signal IIf with the same half-inhibition time of 1 min, leaving signal IIs unaffected. (iv) It was inferred that the putative redox-active histidine is essential for the photooxidation of coordinated Mn2+, the probable initial step of photoactivation, and its photodamage results in the loss of the capabilities of photoactivation and AT-band emission. Based on these, a scheme of electron transfer on the donor side of PSII involving histidine oxidation via Z+ is proposed.     

Composition and function of cytochrome b559 in reaction centers of photosystem II of green plants

A review of a recent study of the spectral and thermodynamic properties of cytochrome b559 as well as of the electron transfer between b559 and photosystem II reaction center cofactors in isolated D1/D2/cytochrome b559 complex RC-2 is presented. Attention is paid to the existence of intermediary-potential (IP, +150 mV) and extra-low-potential (XLP, –45 mV) hemes located close to the acceptor (quinone) and donor (P680) sides of the reaction center cofactors, respectively. These hemes found in isolated RC-2 probably correspond to the high-potential and low-potential hemes in chloroplasts, respectively. The above location of the hemes is believed to allow the photoreduction of the XLP heme and photooxidation of the IP heme. The electron transfer between the two hemes is discussed in terms of the cyclic electron flow and possible involvement in water splitting.     

Electron transfer in photosystem II at cryogenic temperatures

The photochemistry in photosystem II of spinach has been characterized by electron paramagnetic resonance (EPR) spectroscopy in the temperature range of 77-235 K, and the yields of the photooxidized species have been determined by integration of their EPR signals. In samples treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), a single stable charge separation occurred throughout the temperature range studied as reflected by the constant yield of the Fe(II)-QA-EPR signal. Three distinct electron donation pathways were observed, however. Below 100 K, one molecule of cytochrome b559 was photooxidized per reaction center. Between 100 and 200 K, cytochrome b559 and the S1 state competed for electron donation to P680+. Photooxidation of the S1 state occurred via two intermediates: the g = 4.1 EPR signal species first reported by Casey and Sauer [Casey, J. L., & Sauer, K. (1984) Biochim. Biophys. Acta 767, 21-28] was photooxidized between 100 and 160 K, and upon being warmed to 200 K in the dark, this EPR signal yielded the multiline EPR signal associated with the S2-state. Only the S1 state donated electrons to P680+ at 200 K or above, giving rise to the light-induced S2-state multiline EPR signal. These results demonstrate that the maximum S2-state multiline EPR signal accounts for 100% of the reaction center concentration. In samples where electron donation from cytochrome b559 was prevented by chemical oxidation, illumination at 77 K produced a radical, probably a chlorophyll cation, which accounted for 95% of the reaction center concentration. This electron donor competed with the S1 state for electron donation to P680+ below 100 K.(ABSTRACT TRUNCATED AT 250 WORDS)     

An Approach to a Function of Photorespiration in C3 Plants

Intact attached leaves of wheat were illuminated at 2000 μmol m-2·s-1 in CO2-free gas for 3 hours, inhibition percentage of photosynthesis in these leaves by illumination was related lo oxygen concentration in the gas. (1) The damage to the leaves became less gradually when oxygen concentration rose from 0 to 10%. (2) Almost no damage occurred between 10%–50% O2. (3) The damage appeared again when oxygen concentration exceeded 50%. The duration of CO2 outburst of wheat leaves in CO2-free gas containing 8%–11% O2 was 0nly about 15–30 min. However, no photoinhibition could be observed under this condition. Oxygen also could prevent isolated chloroplasts from the damage by strong light. No matter what concentration of oxygen in CO2-free gas was during photoinhibition treatment, the photodamaged site was always in PSⅡ. It is concluded from the results that the way in which photoinhibition was alleviated by oxygen seems not only to be photorespiration, but also the other unknown mechanisms waich may play more important part in it.     

杂交酸模叶片线粒体交替氧化酶呼吸途径在光破坏防御中的作用

以杂交酸模(Rumex K-1)为试材,研究了不同光强下线粒体交替氧化酶呼吸途径(AOX途径)对酸模叶片光破坏的防御作用.结果表明:在200 μmol·m-2·s-1弱光下,用水杨基羟肟酸抑制AOX途径后,Rumex K-1叶片的PSⅡ实际光化学效率、光合线性电子传递速率以及光合放氧速率均显著下降,非还原性QB反应中心显著升高,加重了叶片的光抑制,而活性氧清除机制上调,避免了活性氧的过量积累,部分缓解了Rumex K-1叶片的光抑制;在800 μmol·m-2·s-1强光下,AOX途径受抑,导致Rumex K-1叶片发生严重的光抑制,而此时活性氧清除机制的上调不足以缓解活性氧过量的积累.无论在强光还是弱光下,AOX途径在Rumex K-1叶片的光破坏防御过程中都起着重要作用,而且在强光下,AOX途径对叶片的光破坏防御作用是叶绿体内其他光破坏防御途径所不能代替的.     

Photooxidation of cytochrome b559 in oxygen-evolving photosystem II.

Cytochrome b559 (cyt b559) is an intrinsic and essential component of the photosystem II (PSII) protein complex, but its function, stoichiometry, and electron-transfer kinetics in the physiological system are not well-defined. In this study, we have used flash-detection optical spectroscopy to measure the kinetics and yields of photooxidation and dark reduction of cyt b559 in untreated, O2-evolving PSII-enriched membranes at room temperature. The dark redox states of cyt b559 and the primary electron acceptor, QA, were determined over the pH range 5.0-8.5. Both the fraction of dark-oxidized cyt b559 and dark-reduced QA increased with increasing acidity. Consistent with these results, an acid-induced drop in pH from 8.5 to 4.9 in a dark-adapted sample caused the oxidation of cyt b559, indicating a shift in the redox state during the dark reequilibration. As expected from the dark redox state of cyt b559, the rate and extent of photooxidation of cyt b559 during continuous illumination decreased toward more acidic pH values. After a single, saturating flash, the rate of photooxidation of cyt b559 was of the same order of magnitude as the rate of S2QA- charge recombination. In untreated PSII samples at pH 8.0 with 42% of cyt b559 oxidized and 15% of QA reduced in the dark, 4.7% of one copy of cyt b559 was photooxidized after one flash with a t1/2 of 540 +/- 90 ms. On the basis of our previous work [Buser, C. A., Thompson, L. K., Diner, B. A., & Brudvig, G. W (1990) Biochemistry 29, 8977] and the data presented here, we conclude that Sn+1, YZ., and P680+ are in redox equilibrium and cyt b559 (and YD) are oxidized via P680+. After a period of illumination sufficient to fully reduce the plastoquinone pool, we also observed the pH-dependent dark reduction of photooxidized cyt b559, where the rate of reduction decreased with decreasing pH and was not observed at pH < 6.4. To determine the direct source of reductant to oxidized cyt b559, we studied the dark reduction of cyt b559 and the reduction of the PQ pool as a function of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) concentration. We find that DCMU inhibits the reduction of cyt b559 under conditions where the plastoquinone pool and QA are reduced. We conclude that QB-. (H+) or QBH2 is the most likely source of the electron required for the reduction of oxidized cyt b559.(ABSTRACT TRUNCATED AT 400 WORDS)     

Carotenoid oxidation in photosystem II.

The oxidation of carotenoid upon illumination at low temperature has been studied in Mn-depleted photosystem II (PSII) using EPR and electronic absorption spectroscopy. Illumination of PSII at 20 K results in carotenoid cation radical (Car+*) formation in essentially all of the centers. When a sample which was preilluminated at 20 K was warmed in darkness to 120 K, Car+* was replaced by a chlorophyll cation radical. This suggests that carotenoid functions as an electron carrier between P680, the photooxidizable chlorophyll in PSII, and ChlZ, the monomeric chlorophyll which acts as a secondary electron donor under some conditions. By correlating with the absorption spectra at different temperatures, specific EPR signals from Car+* and ChlZ+* are distinguished in terms of their g-values and widths. When cytochrome b559 (Cyt b559) is prereduced, illumination at 20 K results in the oxidation of Cyt b559 without the prior formation of a stable Car+*. Although these results can be reconciled with a linear pathway, they are more straightforwardly explained in terms of a branched electron-transfer pathway, where Car is a direct electron donor to P680(+), while Cyt b559 and ChlZ are both capable of donating electrons to Car+*, and where the ChlZ donates electrons when Cyt b559 is oxidized prior to illumination. These results have significant repercussions on the current thinking concerning the protective role of the Cyt b559/ChlZ electron-transfer pathways and on structural models of PSII.     

Beta-carotene redox reactions in photosystem II: electron transfer pathway

A carotenoid (Car), a chlorophyll (Chl(Z)), and cytochrome b(559) (Cyt b(559)) are able to donate electrons with a low quantum yield to the photooxidized chlorophyll, P680(+), when photosystem II (PSII) is illuminated at low temperatures. Three pathways for electron transfer from Cyt b(559) to P680(+) are considered: (a) the "linear pathway" in which Cyt b(559) donates via Chl(Z) to Car, (b) the "branched pathway" in which Cyt b(559) donates via Car and where Chl(Z) is also able to donate to Car, and (c) the "parallel pathway" where Cyt b(559) donates to P680 without intermediate electron carriers and electron donation from Chl(Z) and Car occurs by a competing pathway. Experiments were performed using EPR and spectrophotometry in an attempt to distinguish among these pathways, and the following observations were made. (1) Using PSII with an intact Mn cluster in which Cyt b(559) was preoxidized, Car oxidation was dominant upon illumination at < or =20 K, while electron donation from Chl dominated at >120 K. (2) When Cyt b(559) was prereduced, its light-induced oxidation occurred at < or =20 K in what appeared to be all of the centers and without the formation of a detectable Car(+) intermediate. The small and variable quantity of Car(+) photoinduced in these experiments can be attributed to the residual centers in which Cyt b(559) remained oxidized prior to illumination. (3) The relative rates for irreversible electron donation from Cyt b(559) and Car were determined indirectly at 20 K by monitoring the flash-induced loss of charge separation (i.e., the accumulation of Cyt b(559)(+)Q(A)(-) or Car(+)Q(A)(-)). Similar yields per flash were observed (13% for Cyt b(559) and 8% for Car), indicating similar donation rates. The slightly lower yield with Car as a donor is attributed at least in part to slow charge recombination occurring from the Car(+)Q(A)(-) radical pair in a fraction of centers. (4) Light-induced oxidation of Cyt b(559) and Car at 20 K was monitored directly by EPR, and the rates were found to be indistinguishable. The parallel pathway predicts that when both Cyt b(559) and Car are prereduced, the relative amounts of Cyt b(559)(+) and Car(+) produced upon illumination at 20 K should depend directly on their relative electron donation rates. The measured similarity in the donation rates thus predicts comparable yields of oxidation for both donors. However, what is observed experimentally is that Cyt b(559) oxidation occurs almost exclusively, and this argues strongly against the parallel pathway. The lack of Car(+) as a detectable intermediate is attributed to rapid electron transfer from Cyt b(559) to Car(+). The trapping of Car(+) at low temperature when Cyt b(559) is preoxidized but its absence when Cyt b(559) is prereduced is taken as an argument against the simple linear pathway. Overall, the data reported here and previously favor the branched pathway over the linear pathway, while the parallel pathway is thought to be unlikely. Structural considerations provide further arguments in favor of the branched model.     

Photosystem II Excitation Pressure and Development of Resistance to Photoinhibition (I. Light-Harvesting Complex II Abundance and Zeaxanthin Content in Chlorella vulgaris)

The basis of the increased resistance to photoinhibition upon growth at low temperature was investigated. Photosystem II (PSII) excitation pressure was estimated in vivo as 1 - qp (photochemical quenching). We established that Chlorella vulgaris exposed to either 5[deg]C/150 [mu]mol m-2 s-1 or 27[deg]C/2200 [mu]mol m-2 s-1 experienced a high PSII excitation pressure of 0.70 to 0.75. In contrast, Chlorella exposed to either 27[deg]C/150 [mu]mol m-2 s-1 or 5[deg]C/20 [mu]mol m-2 s-1 experienced a low PSII excitation pressure of 0.10 to 0.20. Chlorella grown under either regime at high PSII excitation pressure exhibited: (a) 3-fold higher light-saturated rates of O2 evolution; (b) the complete conversion of PSII[alpha] centers to PSII[beta] centers; (c) a 3-fold lower epoxidation state of the xanthophyll cycle intermediates; (d) a 2.4-fold higher ratio of chlorophyll a/b; and (e) a lower abundance of light-harvesting polypeptides than Chlorella grown at either regime at low PSII excitation pressure. In addition, cells grown at 5[deg]C/150 [mu]mol m-2 s-1 exhibited resistance to photoinhibition comparable to that of cells grown at 27[deg]C/2200 [mu]mol m-2 s-1 and were 3- to 4-fold more resistant to photoinhibition than cells grown at either regime at low excitation pressure. We conclude that increased resistance to photoinhibition upon growth at low temperature reflects photosynthetic adjustment to high excitation pressure, which results in an increased capacity for nonradiative dissipation of excess light through zeaxanthin coupled with a lower probability of light absorption due to reduced chlorophyll per cell and decreased abundance of light-harvesting polypeptides.     

Action Spectrum for Photoactivation of the Water-splitting System in Plastids of Intermittently Illuminated Wheat Leaves

The chloroplasts from wheat leaves developed under intermittent illumination (1 ms light + 12 min dark) were able to photoreduce DPIP with DPC as electron donor but unable to photoreduce DPIP with water as electron donor. On exposure of these leaves to continuous light, the Hill activity with water as electron donor was rapidly induced. The photoactivation was sensitive to the treatment with DCMU prior to exposure to continuous light. The action spectrum for the photoactivation showed a sharp band at 680 nm with a distinct shoulder at 650 nm, and was similar to the absorption spectrum of photosytem-2 particles. These data suggest that the electron transfer driven by photosystem 2 is essential for the activation of the water-splitting system in the chloroplasts of intermittently illuminated leaves.     

Photoinhibition and Photoprotection in Ginkgo biloba leaves: Influence of Temperature,CO2 and O2

In midday ginkgo ( Ginkgo biloba L. ) leaves have to bear photon flux density over 1 400 μmol·m-2·s-l in combination with high temperatures around 35℃ at natural habitat. They show typical midday depression of stomatal conductance and of CO2 assimilation rate. The zeaxanthin changes with light intensity during the day. The influence of the combination of strong light and temperature on photoinhibition was also examined in the laboratory. A low CO2 internal conductance (31 mmol· m- 2·s- 1 ) was found in ginkgo leaves, which had been exposed to excessive light at temperature between 15 ℃ and 35 ℃ with reduced CO2 (80 μL·L-l) or oxygen (2%) for 2 h, causing a low CO2 concentration at the carboxylation site and a high proportion of photorespimtion. The ratio of electron transport to CO2 fixation was rather high in ginkgo ( 16 e- /CO2 at 25 ℃ ) as compared with other plants. It increased with temperature also in 2% 02 which could not be explained solely as due to change of photorespimtion. The reduction of oxygen in 340 or 80 μL·L- 1 CO2 had no effect on the extent of photoinhibition at all temperatures, which indicated that eleetron flow caused by photorespiration in excess light was negligible in protective effect in ginkgo leaves. However, a decreased CO2 coneentration increased photoinhibition, especially at high temperature. It is concluded that the dissipation of excessive excitation energy in the PS II antennae through the xanthophyll cycle may be the major protective mechanism to preventing from the deteriorated effects of strong light in ginkgo leaves.     

Light-induced degradation of cytochrome b559 during photoinhibition of the photosystem II reaction center.

The behaviour of cytochrome (cyt) b559 during acceptor- and donor-side photoinhibition has been investigated in oxygen-evolving and non-evolving photosystem II (PSII) membranes. Strong illumination at 20 degrees C under aerobiosis induced a strong decrease in the absorbance of the cyt b559 alpha-band in the two preparations. This absorbance decline was observed only in non-oxygen-evolving PSII samples when illumination was performed under aerobiosis but at 4 degrees C, or under anaerobiosis at 20 degrees C. These results suggest that acceptor-side photoinhibition induces the degradation of cyt b559 by a mechanism related to an enzymatic reaction mediated by singlet oxygen. Donor-side photoinhibition may induce, however, a non-enzymatic photocleavage of the protein.     

Photoreactions of Cytochrome b-559 and cyclic electron flow in photosystem II of intact chloroplasts.

The high potential cytochrome b-559 of intact spinach chloroplasts was photooxidized by red light with a high quantum efficiency and by far-red light with a very low quantum efficiency, when electron flow from water to Photosystem II was inhibited by a carbonyl cyanide phenylhydrazone (FCCP or CCP). Dithiothreitol, which reacts with FCCP or CCCP, reversed the photooxidation of cytochrome b-559 and restored the capability of the chloroplasts to photoreduce CO2 showing that the FCCP/CCCP effects were reversible. The quantum efficiency of cytochrome b-559 photooxidation by red or far-red light in the presence of FCCP was increased by 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone which blocks oxidation of reduced plastoquinone by Photosystem I. When the inhibition of water oxidation by FCCP or CCP was decreased by increased light intensities, previously photooxidized cytochrome b-559 was reduced. Red light was much more effective in photoreducing oxidized high potential cytochrome b-559 than far-red light. The red/far-red antagonism in the redox state of cytochrome b-559 is a consequence of the different sensitivity of the cytochrome to red and far-red light and does not indicate that the cytochrome is in the main path of electrons from water to NADP. Rather, cytochrome b-559 acts as a carrier of electrons in a cyclic path around Photosystem II. The redox state of the cytochrome was shifted to the oxidized side when electron transport from water became rate-limiting, while oxidation of water and reduction of plastoquinone resulted in its shifting to the reduced side.     

Redox changes of cytochrome b(559) in the presence of plastoquinones

We have found that short chain plastoquinones effectively stimulated photoreduction of the low potential form of cytochrome b(559) and were also active in dark oxidation of this cytochrome under anaerobic conditions in Triton X-100-solubilized photosystem II (PSII) particles. It is also shown that molecular oxygen competes considerably with the prenylquinones in cytochrome b(559) oxidation under aerobic conditions, indicating that both molecular oxygen and plastoquinones could be electron acceptors from cytochrome b(559) in PSII preparations. alpha-Tocopherol quinone was not active in the stimulation of cytochrome photoreduction but efficiently oxidized it in the dark. Both the observed photoreduction and dark oxidation of the cytochrome were not sensitive to 3-(3,4-dichlorophenyl)-1, 1-dimethylurea. It was concluded that both quinone-binding sites responsible for the redox changes of cytochrome b(559) are different from either the Q(A) or Q(B) site in PSII and represent new quinone-binding sites in PSII.     

Comparative EPR and thermoluminescence study of anoxic photoinhibition in Photosystem II particles

Photosystem II particles were exposed to 800 W m^–2 white light at 20 °C under anoxic conditions. The F_o level of fluorescence was considerably enhanced indicating formation of stable-reduced forms of the primary quinone electron acceptor, Q_A. The F_m level of fluorescence declined only a little. The g=1.9 and g=1.82 EPR forms characteristic of the bicarbonate-bound and bicarbonate-depleted semiquinone-iron complex, Q_A ^–Fe²⁺, respectively, exhibited differential sensitivity against photoinhibition. The large g=1.9 signal was rapidly diminished but the small g=1.82 signal decreased more slowly. The S₂-state multiline signal, the oxygen evolution and photooxidation of the high potential form of cytochrome b-559 were inhibited approximately with the same kinetics as the g=1.9 signal. The low potential form of oxidized cytochrome b-559 and Signal II_slow arising from Tyr_D ⁺ decreased considerably slower than the g=1.9 semiquinone-iron signal. The high potential form of oxidized cytochrome b-559 was diminished faster than the low potential form. Photoinhibition of the g=1.9 and g=1.82 forms of Q_A was accompanied with the appearance and gradual saturation of the spin-polarized triplet signal of P 680. The amplitude of the radical signal from photoreducible pheophytin remained constant during the 3 hour illumination period. In the thermoluminescence glow curves of particles the Q band (S₂Q_A ^– charge recombination) was almost completely abolished. To the contrary, the C band (Tyr_D ⁺Q_A ^– charge recombination) increased a little upon illumination. The EPR and thermoluminescence observations suggest that the Photosystem II reaction centers can be classified into two groups with different susceptibility against photoinhibition.Abbreviations C band thermoluminescence band associated with Tyr-D⁺Q _a ^– charge recombination - Chl chlorophyll - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - EPR electron paramagnetic resonance - F_o initial fluorescence - F_m maximum fluorescence - Q band thermoluminescence band originating from S₂Q _a -charge recombination - Q _a the primary quinone electron acceptor of PS II - P 680 the primary electron donor chlorophyll of PS II - S₂ oxidation state of the water-splitting system - Phe pheophytin - TL thermoluminescence - Tyr _d redox active tyrosine-160 of the D₂ protein     

Study of Diurnal Changes in Photosynthetic Rate and Quantum Efficiency of Grapevine Leaves and Their Utilization in Canopy Management

Photosynthetic rate and quatum efficiency of grapevine (Vitis vinifera L. cv. Sauvignon blanc) leaves were measured under the field with ample soil water supply, and in phytotron with ample supply of water and mineral nutrients, constant air humidity and CO2 concentration, and optimum air temperature, respectively. Under field conditions CO2 assimilation quantum efficiency of leaves reached its maximum in the morning, which was followed by continuous decrease and midday depression. The leaves intercepting more light energy in the morning showed a higher quantum efficiency. Those leaves subjected continuously to strong irradiance exhibited a more obvious and longer midday depression. Reduction of leaf light interception around midday could reduce midday depression. Shaded leaves had a higher quantum efficiency than leaves under direct sunlight. The diurnal changes in photosynthetic rate and quantum efficiency of leaves were shown to be closely related to the variations in mesophyll resistance to CO2. In phytotron experiments the photosynthetic quantum efficiency of leaves was reduced after a certain period of illumination not only at 1200 μmol · m-2 · s-1 PFD, higher than the saturating light of vine leaves (≈1000 μmol · m-2 · s-1), which was caused by "photoinhibition”, but also at 800 and 200μmol · m-2 · s-1, which was similar to "photoinhibition”. But photosynthetic quantum efficiency of leaves exposed continuously to a very weak PFD (100 μmol · m -2 · s-1) remained contant. The diurnal changes in mesophyll resistance to CO2 of vine leaves could be partly related to photoinhibition. It is considered that, under field conditions without soil water limitation, midday depression of vine leaf photosynthesis could be a result of an increase of the mesophyll resistance induced by multiple effects of strong light, high temperature and low humidity. A higher light interception by canopy plane in the morning may be advantageous to exploit higher photosynthetic potentiality of leaves, but a lower light interception in the middle of day may reduce midday depression. The north-south orientation plane can provide optimum light regime and improve photosynthetic environment in vineyards.     

A theoretical study on effect of the initial redox state of cytochrome b559 on maximal chlorophyll fluorescence level (F(M)): implications for photoinhibition of photosystem II

In this work, we extended the reversible radical pair model which describes energy utilization and electron transfer up to the first quinone electron acceptor (Q(A)) in photosystem II (PSII), by redox reactions involving cytochrome (cyt) b559. In the model, cyt b559 accepts electrons from the reduced primary electron acceptor in PSII, pheophytin, and donates electrons to the oxidized primary electron donor in PSII (P680+). Theoretical simulations of chlorophyll fluorescence rise based on the model show that the maximal fluorescence, F(M), increases with an increasing amount of initially reduced cyt b559. In this work we applied, the first to our knowledge, metabolic control analysis (MCA) to a model of reactions in PSII. The MCA was used to determine to what extent the reactions occurring in the model control the F(M) level and how this control depends on the initial redox state of cyt b559. The simulations also revealed that increasing the amount of initially reduced cyt b559 could protect PSII against photoinhibition. Also experimental data, which might be used to validate our theory, are presented and discussed.     

Photoinhibition of hydroxylamine-extracted photosystem II membranes: identification of the sites of photodamage.

Electron paramagnetic resonance (EPR) analyses (g = 2 region) and optical spectrophotometric analyses of P680+ were made of NH2OH-extracted photosystem II (PSII) membranes after various durations of weak-light photoinhibition, in order to identify the sites of damage responsible for the observed kinetic components of the loss of electron transport [Blubaugh, D.J., & Cheniae, G.M. (1990) Biochemistry 29, 5109-5118]. The EPR spectra, recorded in the presence of K3Fe(CN)6, gave evidence for rapid (t1/2 = 2-3 min) and slow (t1/2 = 3-4) losses of formation of the tyrosyl radicals YZ+ and YD+, respectively, and the rapid appearance (t1/2 = 0.8 min) of a 12-G-wide signal, centered at g = 2.004, which persisted at 4 degrees C in subsequent darkness in rather constant abundance (approximately 1/2 spin per PSII). This latter EPR signal is correlated with quenching of the variable chlorophyll a fluorescence yield and is tentatively attributed to a carotenoid (Car) cation. Exogenous reductants (NH2OH greater than or equal to NH2NH2 greater than DPC much greater than Mn2+) were observed to reduce the quencher, but did not reverse other photoinhibition effects. An additional 10-G-wide signal, tentatively attributed to a chlorophyll (Chl) cation, is observed during illumination of photoinhibited membranes and rapidly decays following illumination. The amplitude of formation of the oxidized primary electron donor, P680+, was unaffected throughout 120 min of photoinhibition, indicating no impairment of charge separation from P680, via pheophytin (Pheo), to the first stable electron acceptor, QA. However, a 4-microsecond decay of P680+, reflecting YZ----P680+, was rapidly (t1/2 = 0.8 min) replaced by an 80-140 microsecond decay, presumably reflecting QA-/P680+ back-reaction. Photoinhibition caused no discernible decoupling of the antenna chlorophyll from the reaction center complex. We conclude that the order of susceptibility of PSII components to photodamage when O2 evolution is impaired is Chl/Car greater than YZ greater than YD much greater than P680, Pheo, QA.     

Structure and Photosynthetic Characteristics of Awns of Wheat and Barley

The surface and the cross section of awns of wheat and barley were examined by scanning electron microscopy,ultrastructure of cells were observed under a transmisson electron microscope and the photosynthetic rates were measured with an oxygen, electrode and infra-red CO2 analyser. The main results were as follows :The cross section of wheat awn appeared to be acutely trianglular whereas that of barley awn was obtusely triangular. There were rows of stomota on either side of epidermis in both wheat and barley awns. Under the stomatic band there were green tissues. The green cells in the awn were differentiated from the parenchyma cells . The mature green cells possessed papillae which were rich in chloroplasts and mitochondria. The tamella system in chloroplasts was well developed and contained many starch grains. There were three vascular bundles in each awn. The sheath cells near the green tissues contained chloroplasts. The photosynthate in the green cells might pass through the sheath cells and companion cells to sieve elements. The highest photosynthetic rate of the awn was seen at the flowering stage ,reaching about 20 μmol CO2·m-2·s-1. The light compensation point was 70—80 μE·m-2· s-1. The light saturation point was about 1500 μE·m-2·s-1. The CO2 compensation point was 50—60 ppm and the CO2 saturation point was about 900ppm . The photosynthetic rate and stomatal conductance were easily effected by CO2 concentration, light intensity and the duration of illumination . There was a positive correlation between the photosynthetic rate and the chloro-phyll content in the awns. The CO2-releasing rate in photorespiration of awn was about 4–5 μmol CO2·m-2·s-1.