Photosynthetic energy storage of Photosystems I and II in the spectral range of photosynthetically active radiation in intact sugar maple leaves

The relative activity of Photosystems (PS) I and II in the spectral range between 400 and 720 nm was studied by measuring photosynthetic energy storage (ES) of an intact sugar maple leaf using photoacoustic spectroscopy. ES, determined with a modulated (80 Hz) monochromatic light beam in the presence of saturating intensity of background non-modulated white light, indicated the total energy stored by both photosystems (ES_T). Using background far-red light, ES of PS I (ES_{PS I}) was quantified. ES_{PS II} was derived from ES_T-ES_{PS I}. ES_T dependence on intensity and wavelength of modulated light was studied at 470, 560, 640 and 680 nm. ES_T was maximum in red light and minimum in blue light. It decreased with an increase in modulated light intensity. The ratio ES_{PS II}/ES_{PS I}, measured at 640 nm, remained nearly constant with an increase in modulated light intensity. The relative quantum yield of ES_T spectrum showed two peaks around 610 and 660 nm, and declined sharply after 680 nm, revealing a clear red drop. ES_{PS I} spectrum presented peaks around 610 and 670 nm, and a minimum between 440 and 470 nm. ES_{PS I} was observed beyond 700 nm up to 720 nm, indicating the energy stored by cyclic electron transport. ES_{PS II} spectrum showed broad peaks, around 460, 490, 600 and 660 nm, and a shoulder between 530 and 560 nm. ES_{PS II} was always higher than ES_{PS I} between 400 and 690 nm and reached zero around 700 nm.Abbreviations ES energy storage - ES_{PS I} energy storage of PS I - ES_{PS II} energy storage of PS II - ES_T energy storage of PS I and PS II - PA photoacoustic - PS I Photosystem I - PS II Photosystem II - Q_m PA signal in the absence of any background light - Q_ma PA signal in the presence of background white light - Q_mfrl PA signal in the presence of background far-red light - S/N signal to noise     

A photoacoustic study of water infiltrated leaves

Photoacoustic measurements of photosynthetic energy storage were conducted on water infiltrated pea and sugar maple leaves. The samples were vacuum infiltrated with pure water or with a suitable buffer. The use of such methodology permitted an accurate determination of the energy storage parameter at low modulation frequencies, where in non-infiltrated leaves oxygen evolution dominates the photoacoustic signal and does not allow energy storage measurements. Differences between infiltration media were not essential, however the use of pure water as infiltration medium sometimes caused instability of the measured energy storage, particularly at longer experimental time. Values of energy storage in individual samples ranged mostly between 0.2 to 0.35. Measured as a function of the modulation frequency, energy storage was found to be constant from about 10 to 200 Hz for pea leaves. In sugar maple leaves, the energy storage slightly increased between 100 and 500 Hz. Obtaining an accurate value for energy storage also allowed an accurate estimation of the O₂ evolution contribution to the photoacoustic signal of an unfiltrated leaf. In a maple leaf its frequency dependence showed only the effect of diffusion in the entire frequency range (10–500 Hz). Energy storage transients were observed after long periods (ca. 1/4-2 hrs) of dark adaptation upon the transition to light. In this case the initial energy storage was roughly about 1/2 that of the steady state value indicating strong PS I activity, while PS II was transiently incompetent. Energy-storage increased during illumination in a way to correspond to photosynthetic induction events as previously measured by fluorescence and O₂ evolution. Transients in energy storage were also found following high light to low light transitions (i.e., switch off of the saturating background light), that paralleled similar transients in oxygen evolution, showing initial transient inactivation followed by progressive reactivation of PS II.Abbreviations ES energy storage - PA photoacoustic(s) - PTR photothermal radiometry     

Regulation of the distribution of excitation energy in Ochromonas danica,an organism containing a chlorophyll-A/C/carotenoid light harvesting antenna

A chlorophyll a, c-fucoxanthin pigment-protein complex8 functions as the major light harvesting antenna in the Chrysophyte Ochromonas danica. The regulated distribution of excitation energy between the two photosystems was investigated in these organisms and was shown to be strongly wavelength dependent. A light state transition was induced by pre-illumination of cells using light 2 (640 nm) and light 1 (700 nm) of equal absorbed intensity, and detected by reversible changes in the 77 K chlorophyll fluorescence emission spectra. Peaks at 690 nm and 720 nm in the low temperature spectra are most likely associated with PS2 and PS1 respectively. A room temperature fluorescence emission at 680 nm induced by modulated light 2 (500 nm) was strongly quenched in the presence of background light 1 (720 nm). Removal of light 1 led to an increase in fluorescence followed by a slow quenching. The room temperature fluorescence changes were directly correlated with changes in the 77 K emission spectra that indicated a change in the distribution of excitation energy between the two photosystems. It was established that DCMU (1 mol) prevented the state 2. The conversion to state 1 followed a simple photochemical dose dependence and had a half-time of 20 s-1.5 min at 6 W m^-2. In contrast, the conversion to state 2 was independent of light intensity. These data indicate that O. danica undergoes a light state transition in response to the preferential excitation of PS2 or PS1.Abbreviations PS2 photosystem 2 - PS1 photosystem 1 - LHC light harvesting chlorophyll a/b protein - fx fucoxanthin - PQ plastoquinone - DCMU 3-(3,4-dichlorophenyl)-1,1-dimethyl urea     

Simultaneous detection of photosynthetic energy storage and oxygen evolution in leaves by photothermal radiometry and photoacoustics

We have measured simultaneously the photothermal radiometry and the photoacoustic signals from intact leaves. We have confirmed that while the former senses that part of the modulated absorbed radiation not used in photosynthesis, but converted into heat, the latter, at low modulation frequencies, senses not only this heat but also the modulated oxygen evolution resulting from photosynthesis in the leaf. When photosynthetic activity is saturated upon additional excitation with strong non-modulated light, the photothermal radiometry signal increases (virtually all absorbed modulated light being converted into heat), while at the same time the photoacoustic signal decreases, because virtually no modulated oxygen evolution occurs any more. At higher modulation frequencies the behaviour of the photoacoustic signal closely follows that of the photothermal radiometry signal. We have used combined photothermal radiometry / photoacoustic measurements to estimate directly the yield of chemical energy storage in various plant species which applies for different times after excitation. Measurement of light saturation curves for wheat and Siberian pea bush leaves and of action spectra for the latter confirm the similarity between photothermal radiometry and high-frequency photoacoustic signals, and their difference from the low-frequency photoacoustic signal. Combined use of photothermal radiometry (or high-frequency photoacoustics) and low-frequency photoacoustics can thus provide more information than any one method alone. Experiments on intact chloroplasts and on a blue-green alga demonstrate that photothermal radiometry and photoacoustic methodologies can also be used for these tissues.     

Detection of photosynthetic energy storage in a photosystem I reaction center preparation by photoacoustic spectroscopy

Thermal emission and photochemical energy storage were examined in photosystem I reaction center/core antenna complexes (about 40 Chl a/P700) using photoacoustic spectroscopy. Satisfactory signals could only be obtained from samples bound to hydroxyapatite and all samples had a low signal-to-noise ratio compared to either PS I or PS II in thylakoid membranes. The energy storage signal was saturated at low intensity (half saturation at 1.5 W m^-2) and predicted a photochemical quantum yield of >90%. Exogenous donors and acceptors had no effect on the signal amplitudes indicating that energy storage is the result of charge separation between endogenous components. Fe(CN)₆ ^-3 oxidation of P700 and dithionite-induced reduction of acceptors F_A-F_B inhibited energy storage. These data are compatible with the hypothesis that energy storage in PS I arises from charge separation between P700 and Fe-S centers F_A-F_B that is stable on the time scale of the photoacoustic modulation. High intensity background light (160 W m^-2) caused an irreversible loss of energy storage and correlated with a decrease in oxidizable P700; both are probably the result of high light-induced photoinhibition. By analogy to the low fluorescence yield of PS I, the low signal-to-noise ratio in these preparations is attributed to the short lifetime of Chl singlet excited states in PS I-40 and its indirect effect on the yield of thermal emission.Abbreviations FFT fast Föurier transform - HA hydroxyapatite - I₅₀ half saturation intensity for energy storage - PA photoacoustic - PS photosystem - PS I-40 photosystem I reaction center/core antenna complex containing about 40 Chl a/P700 - 201-1 photoacoustic energy storage signal - S/N signal-to-noise     

Photoinhibition of photosynthesis in chilled potato leaves is not correlated with a loss of Photosystem-II activity

When 23 °C-grown potato leaves (Solanum tuberosum L.) were irradiated at 23 °C with a strong white light, photosynthetic electron transport and Photosystem-II (PS II) activity were inhibited in parallel. When the light treatment was given at a low temperature of 3 °C, the photoinhibition of photosynthesis was considerably enhanced, as expected. Surprisingly, no such stimulation of photoinhibition was observed with respect to the PS II function. A detailed functional analysis of the photosynthetic apparatus, using in-vivo fluorescence, absorbance, oxygen and photoacoustic measurements, and artificial electron donors/acceptors, showed a pronounced alteration of PS I activity during light stress at low temperature. More precisely, it was observed that both the pool of photooxidizeable reaction center pigment (P₇₀₀) of PS I and the efficiency of PS I to oxidize P₇₀₀ were dramatically reduced. Loss of P₇₀₀ activity was shown to be essentially dependent on atmospheric O₂ and to require a continued flow of electrons from PS II, suggesting the involvement of the superoxide anion radical which is produced by the interaction of O₂ and the photosynthetic electron-transfer chain through the Mehler reaction. Mass spectrometric measurements of O₂ exchange by potato leaves under strong illumination did not reveal, however, any stimulation of the Mehler reaction at low temperature, thus leading to the conclusion that O₂ toxicity mainly resulted from a chilling-induced inhibition of the scavenging system for O₂-radicals. Support for this interpretation was provided by the light response of potato leaves infiltrated with an inhibitor (diethyldithiocarbamate) of the chloroplastic Cu-Zn superoxide dismutase. It was indeed possible to simulate the differential inhibition of the PS II photochemical activity and the linear electron transport observed during light stress at low temperature by illuminating at 23 °C diethyldithiocarbamate-poisoned leaves. The experimental data presented here suggests that (i) the previously reported resistance of PS I to photoinhibition damage in-vivo is not an intrinsic property of PS I but results from efficient protective systems against O₂ toxicity, (ii) PS I is photoinhibited in chilled potato leaf due to the inactivation of this PS I defence system and (iii) PS I is more sensitive to superoxide anion radicals than PS II.Abbreviations PS - Photosystem - E - Emerson enhancement - _open ^p and ^P maximal and actual quantum yields of PS II photochemistry - DDC - diethyldithiocarbamate - Q_A and Q_B - primary and secondary (quinone) electron acceptors of PS II - P₆₈₀ and P₇₀₀ - reaction center pigments of PS II and PS I, respectively - SOD - superoxide dismutase     

In vivo studies of gross photosynthesis in attached leaves by means of photothermal radiometry

In photothermal radiometry, heat radiation from an illuminated object, in synchronism with incident chopped light, is observed using an infrared detector with suitable electronics. By thus measuring the heat released during pulse-wise irradiation of leaves, conclusions can be drawn as to the gross efficiency of photosynthesis: More heat means less photochemically stored energy. Saturation of photosynthesis, by employing additional strong continuous-wave background light, affords an internal photothermal radiometry signal reference corresponding to the photochemical zero efficiency level, against which the signal in the absence of saturation can be compared. Through such means, gross energy storage efficiencies approaching 30% have been observed in Caragana arborescens Lam. at low light intensities. Several other examples are given, including measurements on dark-adapted leaves and leaves infiltrated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea, to support our conclusion that photothermal radiometry provides a powerful new method for in vivo studies of photosynthesis in whole, attached leaves.     

Photoacoustic Study of Changes in the Energy Storage of Photosystems I and II during State 1-State 2 Transitions

Using photoacoustic spectroscopy, state 1-state 2 transitions were demonstrated in vivo in intact sugar maple leaves (Acer saccharum Marsh.) by following the changes in energy storage of photosystems (PS) I and II. Energy storage measured with 650 nm modulated light (light 2) in the presence of background white light indicated the total energy stored by both photosystems (ES_t), and in the presence of background far-red light showed the energy stored by PSI (ES_psi). The difference between ES_t and ES_psi gave the energy stored by PSII (ES_psii). While ES_t remained nearly constant during state transitions, both ES_psi and ES_psii changed considerably. The ratio of ES_psii to ES_psi, an indicator of the energy distribution between the two photosystems, decreased or increased during transition to state 2 or state 1, respectively. State transitions were completed in about 20 min and were fully reversible. During transition from state 1 to state 2, the fraction of excitation energy gained by PSI was nearly equal to that lost by PSII. This fraction of excitation energy transferred from PSII to PSI accounted for about 5% of the absorbed light (fluorescence is not considered), 19% of ES_t, 34% of ES_psii, and 43% of ES_psi in state 2. NaF treatment inhibited the transition to state 1. Data in the present study confirm the concept of changes in absorption cross-section of photosystems during state transitions.     

Femtosecond primary charge separation in Synechocystis sp. PCC 6803 photosystem I

The ultrafast (< 100 fs) conversion of delocalized exciton into charge-separated state between the primary donor P700 (bleaching at 705 nm) and the primary acceptor A₀ (bleaching at 690 nm) in photosystem I (PS I) complexes from Synechocystis sp. PCC 6803 was observed. The data were obtained by application of pump-probe technique with 20-fs low-energy pump pulses centered at 720 nm. The earliest absorbance changes (close to zero delay) with a bleaching at 690 nm are similar to the product of the absorption spectrum of PS I complex and the laser pulse spectrum, which represents the efficiency spectrum of the light absorption by PS I upon femtosecond excitation centered at 720 nm. During the first ∼ 60 fs the energy transfer from the chlorophyll (Chl) species bleaching at 690 nm to the Chl bleaching at 705 nm occurs, resulting in almost equal bleaching of the two forms with the formation of delocalized exciton between 690-nm and 705-nm Chls. Within the next ∼ 40 fs the formation of a new broad band centered at ∼ 660 nm (attributed to the appearance of Chl anion radical) is observed. This band decays with time constant simultaneously with an electron transfer to A₁ (phylloquinone). The subtraction of kinetic difference absorption spectra of the closed (state P700⁺A₀A₁) PS I reaction center (RC) from that of the open (state P700A₀A₁) RC reveals the pure spectrum of the P700⁺A₀⁻ ion-radical pair. The experimental data were analyzed using a simple kinetic scheme: An* [(PA₀)*A₁ P⁺A₀⁻A₁] P⁺A₀A₁⁻, and a global fitting procedure based on the singular value decomposition analysis. The calculated kinetics of transitions between intermediate states and their spectra were similar to the kinetics recorded at 694 and 705 nm and the experimental spectra obtained by subtraction of the spectra of closed RCs from the spectra of open RCs. As a result, we found that the main events in RCs of PS I under our experimental conditions include very fast (< 100 fs) charge separation with the formation of the P700⁺A₀⁻A₁ state in approximately one half of the RCs, the ∼ 5-ps energy transfer from antenna Chl* to P700A₀A₁ in the remaining RCs, and ∼ 25-ps formation of the secondary radical pair P700⁺A₀A₁⁻.     

Fluorescence detected magnetic resonance of the primary donor and inner core antenna chlorophyll in Photosystem I reaction centre protein: Sign inversion and energy transfer

The Photosystem I reaction centre protein CP1, isolated from barley using polyacrylamide gel electrophoresis showed an EPR (Electron Paramgnetic Resonance) spectrum with the polarisation pattern AEEAAE, typical of the primary donor triplet state ³P700, created via radical pair formation and recombination. ³P700 could also be detected by Fluorescence Detected Magnetic Resonance (FDMR) at _f > 700 nm even in the presence of a large number of chlorophyll antennae. Its zero field splitting parameters, D=282.5×10^-4 cm^-1 and E=38.5×10^-4 cm^-1, were independent of the detection wavelength, and agreed with ADMR (Absorption Detected Magnetic Resonance) and EPR values. The signs of the ³P700 D+E and D-E transitions were positive (increase in fluorescence intensity on applying a resonance microwave field). In contrast, in the emission band 685 < _f < 700 nm FDMR spectra with negative D+E and D-E transitions were detected, and the D value was wavelength-dependent. These FDMR results support an excitation energy transfer model for CP1, derived from time-resolved fluorescence studies, in which two chlorophyll antenna forms are distinguished, with fluorescence at 685 < _f < 700 nm (inner core antennae, F690), and _f > 700 nm (low energy antenna sites, F720), in addition to the P700. The FDMR spectrum in F690 emission can be interpreted as that of ³P700, observed via reverse singlet excitation energy transfer and added to the FDMR spectrum of the antenna triplet states generated via intramolecular intersystem crossing. This would indicate that reversible energy transfer between F690 and P700 occurs even at 4.2 K.Abbreviations Chl chlorophyll - CP1 core chlorophyll protein of Photosystem I - EPR electron paramagnetic resonance - F690, F720 chlorophyll forms having fluorescence maximum at 690–695 and 720 nm, respectively - F(A)(O)DMR fluorescence (absorption) (optical) detected magnetic resonance - FF fluorescence fading - ISC intramolecular intersystem crossing - _f fluorescence emission wave-length - LHC I light harvesting chlorophyll a/b protein of Photosystem I - P700 primary donor of Photosystem I - PS I Photosystem I - RC reaction centre - RP radical pair - SDS sodium dodecyl sulphate - ZFS zero field splitting     

Photosystem I-dependent cyclic electron transport is important in controlling Photosystem II activity in leaves under conditions of water stress

Leaves of the C₃ plant Brassica oleracea were illuminated with red and/or far-red light of different photon flux densities, with or without additional short pulses of high intensity red light, in air or in an atmosphere containing reduced levels of CO₂ and/or oxygen. In the absence of CO₂, far-red light increased light scattering, an indicator of the transthylakoid proton gradient, more than red light, although the red and far-red beams were balanced so as to excite Photosystem II to a comparable extent. On red background light, far-red supported a transthylakoid electrical field as indicated by the electrochromic P₅₁₅ signal. Reducing the oxygen content of the gas phase increased far-red induced light scattering and caused a secondary decrease in the small light scattering signal induced by red light. CO₂ inhibited the light-induced scattering responses irrespective of the mode of excitation. Short pulses of high intensity red light given to a background to red and/or far-red light induced appreciable additional light scattering after the flashes only, when CO₂ levels were decreased to or below the CO₂ compensation point, and when far-red background light was present. While pulse-induced light scattering increased, non-photochemical fluorescence quenching increased and F₀ fluorescence decreased indicating increased radiationless dissipation of excitation energy even when the quinone acceptor Q_A in the reaction center of Photosystem II was largely oxidized. The observations indicate that in the presence of proper redox poising of the chloroplast electron transport chain cyclic electron transport supports a transthylakoid proton gradient which is capable of controlling Photosystem II activity. The data are discussed in relation to protection of the photosynthetic apparatus against photoinactivation.Abbreviations F, F_M, F'_M, F"_M, F₀, F'₀ chlorophyll fluorescence levels - _exc quantum efficiency of excitation energy capture by open Photosystem II - _{PS II} quantum efficiency of electron flow through Photosystem II - P₅₁₅ field indicating rapid absorbance change peaking at 522 nm - P₇₀₀ primary donor of Photosystem I - Q_A primary quinone acceptor in Photosystem II - Q_N non-photochemical fluorescence quenching - Q_q photochemical quenching of chlorophyll fluorescence     

Short-term responses of Photosystem I to heat stress

When 23°C-grown potato leaves (Solanum tuberosum L.) were exposed for 15 min to elevated temperatures in weak light, a dramatic and preferential inactivation of Photosystem (PS) II was observed at temperatures higher than about 38°C. In vivo photoacoustic measurements indicated that, concomitantly with the loss of PS II activity, heat stress induced a marked gas-uptake activity both in far-red light (>715 nm) exciting only PS I and in broadband light (350–600 nm) exciting PS I and PS II. In view of its suppression by nitrogen gas and oxygen and its stimulation by high carbon-dioxide concentrations, the bulk of the photoacoustically measured gas uptake by heat-stressed leaves was ascribed to rapid carbon-dioxide solubilization in response to light-modulated stroma alkalization coupled to PS I-driven electron transport. Heat-induced gas uptake was observed to be insensitive to the PS II inhibitor diuron, sensitive to the plastocyanin inhibitor HgCl₂ and saturated at a rather high photon flux density of around 1200 E m^–2 s^–1. Upon transition from far-red light to darkness, the oxidized reaction center P700⁺ of PS I was re-reduced very slowly in control leaves (with a half time t_1/2 higher than 500 ms), as measured by leaf absorbance changes at around 820 nm. Heat stress caused a spectacular acceleration of the postillumination P700⁺ reduction, with t_1/2 falling to a value lower than 50 ms (after leaf exposure to 48°C). The decreased t_1/2 was sensitive to HgCl₂ and insensitive to diuron, methyl viologen (an electron acceptor of PS I competing with the endogenous acceptor ferredoxin) and anaerobiosis. This acceleration of the P700⁺ reduction was very rapidly induced by heat treatment (within less than 5 min) and persisted even after prolonged irradiation of the leaves with far-red light. After heat stress, the plastoquinone pool exhibited reduction in darkness as indicated by the increase in the apparent Fo level of chlorophyll fluorescence which could be quenched by far-red light. Application (for 1 min) of far-red light to heat-pretreated leaves also induced a reversible quenching of the maximal fluorescence level Fm, suggesting formation of a pH gradient in far-red light. Taken together, the presented data indicate that PS I responded to the heat-induced loss of PS II photochemical activity by catalyzing an electron flow from stromal reductants. Heat-stress-induced PS I electron transport independent of PS II seems to constitute a protective mechanism since block of this electron pathway in anaerobiosis was observed to result in a dramatic photoinactivation of PS I.Abbreviations PFD photon flux density - PS Photosystem - Apt and Aox amplitude of the photothermal and photobaric components of the photoacoustic signal, respectively - P700 reaction center pigment of PS I - Fo and Fm initial and maximal levels of chlorophyll fluorescence, respectively - Fv=Fm Fo-variable chlorophyll fluorescence - Q_A primary (stable) electron acceptor of PS II - DCMU (diuron) 3-(3,4-dichlorophenyl)-1,1-dimethylurea - Cyt cytochrome     

Effect of chromate ions on marine microalgae <Emphasis Type="Italic">Phaeodactylum tricornutum</Emphasis>

Effect of chromate ions on the culture of a marine diatom Phaeodactylum tricornutum was studied using an M-PEA-2 fluorimeter, which carries out simultaneous measurement of fluorescence induction and redox transformations of the P₇₀₀ pigment within a millisecond range. Chromate ions were shown to inhibit electron transport in PS II and decrease the rate of Q_А reduction. This results in decreased values of the quantum yield of electron transport in PS II (?_Eo) and performance index (PI _ABS), lower rates of P700 reduction, and increased energy (DI0/RC) and ΔpH-dependent nonphotochemical quenching (q _E ). Emergence of the slow component of P₇₀₀ reduction was observed, indicating the activation of cyclic transport in the presence of chromate. Performance index (PI _ABS), which was the most sensitive parameter, may be recommended for detection of chromate ions at early stages of their toxic action. The fluorescence parameter F _O is promising application in biotesting to assess the algal growth rates.     

Characterization of P700 as a photochemical quencher in isolated Photosystem I particles using simultaneous measurements of absorbance changes at 830 nm and photoacoustic signal

The relationship between the redox state of P700, the primary donor of PS I, monitored using absorbance changes at 830 nm and photochemical energy storage in PS I reaction centers assayed with the photoacoustic method (PA) was studied in isolated PS I submembrane particles aspirated onto nitrocellulose filters. Several donors have been used to support the electron transport through PS I. NADPH and NADH demonstrated low rates of electron donation to PS I, while ascorbate and ascorbate plus 2,6-dichlorophenolindophenol (DCIP) couple have been found more effective in both P700⁺ reduction and stimulation of the variable component of the PA signal. A linear relationship was found in isolated PS I particles between the (A_830,max – A_830,steady)/A_830,max and (PA_max – PA_steady)/PA_max ratios, which characterized the relative amount of P700 in the reduced state and the relative magnitude of the variable PA component, respectively. That linear relationship was obtained independently from the nature of electron donor used for the reduction of P700⁺. Such linear relationship was also obtained at various wavelengths of modulated light in the range of 660 to 720 nm, only the slope of the linear fits varied with wavelength. It is concluded that reduced P700 act as a photochemical quencher of absorbed energy. Variable thermal dissipation in PS I reaction centers of isolated submembrane particles linearly depends on the amount of reduced P700 and thus constitutes an appropriate indicator of the redox pressure applied to PS I. This revised version was published online in June 2006 with corrections to the Cover Date.     

The cyclic electron pathways around photosystem I in Chlamydomonas reinhardtii as determined in vivo by photoacoustic measurements of energy storage

The photoacoustic technique was used to measure energy storage by cyclic electron transfer around photosystem I in intact Chlamydomonas reinhardtii cells illuminated with far-red light (>715 nm). The in-vivo cyclic pathway was characterized by investigating the effects of various chemicals on energy storage. Participation of plastoquinone and ferredoxin in the cyclic electron flow was confirmed by the complete suppression of energy storage in the presence of the plastoquinol antagonist 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone (DBMIB) and the ferredoxin inhibitors/competitors methylviologen, phenylmercuric acetate and p-benzoquinone. Two alternative electron cycles are demonstrated to operate in vivo. One cycle is sensitive to antimycin A, myxothiazol and 2-(n-heptyl)-4-hydroxyquinoline N-oxide (HQNO) and is catalyzed by ferredoxin which reduces plastoquinone through a route involving cytochrome b ₆ and its protonmotive Q-cycle. The other cycle is unaffected by the above-mentioned inhibitors but is sensitive to N-ethylmaleimide (NEM), an inhibitor of the ferredoxin-NADP reductase, and 2-monophosphoadenosine-5-diphosphoribose (PADR), an analogue of NADP, showing that the electron recycling was mediated by NADPH. Possibly, electrons enter the plastoquinone pool through the action of a NAD(P)H dehydrogenase, which is insensitive to classical inhibitors of the mitochondrial NADH dehydrogenase. Loss of energy storage by photosystem-I-driven cyclic electron transfer in farred light was observed only when antimycin A, myxothiazol or HQNO was used in combination with NEM or PADR. Analysis of the light-intensity dependence and the rate of in-vivo cyclic electron transfer in the presence of various inhibitors indicates that the NADPH-dependent electron-cycle is the preferential cyclic pathway in Chlamydomonas cells illuminated with far-red light.Abbreviations A^max maximal photothermal signal - Cyt cytochrome - DBMIB 2,5-dibromo-3-methyl-6-isopropyl-p-benzoquinone - DCMU (diuron) 3-(3,4-dichlorophenyl)-1,1-dimethylurea - ES photochemical energy storage - FNR ferredoxin NADP⁺ reductase - HQNO 2-(n-heptyl)-4-hydroxyquinoline N-oxide - NEM N-ethylmaleimide - P₇₀₀ reaction-center pigment of PSI - PADR 2-monophosphoadenosine-5-diphosphoribose - pBQ p-benzoquinone - PMA phenylmercuric acetate We are very grateful to Dr. M.-H. Montane (Cadarache, Saint-Paul-lez-Durance, France) for her advice in the electroporation experiments.     

Photoacoustic characteristics of leaves of atrazine-resistant weed mutants

The photosynthetic characteristics of leaves of atrazine-resistant and-susceptible biotypes of several weed species (Solanum nigrum, Senecio vulgaris, Epilobium ciliatum and Chenopodium album) were compared using the photoacoustic method. Analysis of the dependence of the photoacoustic signal of the modulation frequency indicated that, in Solanum, Epilobium and Senecio, the relative quantum yield of O₂ evolution (estimated by the ratio of the amplitude of the O₂ signal, A_OX, to that of the photothermal signal, A_PT) was substantially reduced in the atrazine-resistant mutant, without any changes in the O₂ diffusion characteristics of the leaves. In contrast, in Chenopodium, atrazine-resistance was associated with a concomitant change in and in the leaf diffusion parameters. This latter change suggests that the leaf internal anatomy was modified in the resistant Chenopodium. Measurements of the Emerson enhancement indicated that the reduction of observed in the atrazine-resistant mutants was caused by a marked decrease in the photochemical potential of PS II (). The study of the light intensity dependence of the A_OX/A_PT ratio showed that saturation of O₂ evolution occurred at the same light level (around 2000 mol m^-2 s^-1) in both types of plants. However, the relative maximal rate of O₂ evolution was slightly lower (-10%) in the atrazine-resistant biotype as compared to the wild type. Reduced and light-saturated rate of O₂ evolution were also measured in atrazine-resistant weed biotypes using a conventional Clark-type O₂ electrode.Abbreviations A_OX modulated O₂ evolution component of the photoacoustic signal - A_PT photothermal component of the photoacoustic signal - Atrazine 2-chloro-4-(ethylamino)-6-(isopropylamino)-s-triazine - E Emerson enhancement - PS II and PS I photosystems II and I, respectively - Q_A primary electron acceptor of PS II - Q_B secondary electron acceptor of PS II - quantum yield of O₂ evolution     

Estimation of biophysical characteristics for <Emphasis Type="Italic">Chlamydomonas reinhardtii</Emphasis> pigment mutants with an M-PEA-2 fluorometer

Light green pigment mutants with a reduced chlorophyll b content were constructed in the microalga Chlamydomonas reinhardtii Dangeard. A simultaneous recording of the induction curves for prompt and delayed fluorescence and the redox state of P700 in the microsecond range with a M-PEA-2 fluorometer revealed decreases in the quantum yield of electron transport in PS2 (φE₀) and the performance index (PI_ABS) and increases in the quantum efficiency of energy dissipation (φD₀) and ΔpH-dependent nonphotochemical quenching (qE and NPQ). The light-dependence curves of the fluorescence parameters confirmed a decrease in the coefficient of maximum utilization of light energy (α) for the mutants. However, the mutants showed an adequate rate of electron transport at a medium light intensity under steady-state conditions. The mutations did not directly affect the oxidation reactions of the PS1 pigment (P700) and the decrease in delayed fluorescence. Experience in using the mutants to test polluted waters of Kazakhstan confirmed that the mutants are promising for use in biomonitoring for mutagens.     

Theoretical assessment of alternative mechanisms for non-photochemical quenching of PS II fluorescence in barley leaves

The components of non-photochemical chlorophyll fluorescence quenching (qN) in barley leaves have been quantified by a combination of relaxation kinetics analysis and 77 K fluorescence measurements (Walters RG and Horton P 1991). Analysis of the behaviour of chlorophyll fluorescence parameters and oxygen evolution at low light (when only state transitions — measured as qN_t — are present) and at high light (when only photoinhibition — measured as qN_i — is increasing) showed that the parameter qN_t represents quenching processes located in the antenna and that qN_i measures quenching processes located in the reaction centre but which operate significantly only when those centres are closed. The theoretical predictions of a variety of models describing possible mechanisms for high-energy-state quenching, measured as the residual quenching, qN_e, were then tested against the experimental data for both fluorescence quenching and quantum yield of oxygen evolution. Only one model was found to agree with these data, one in which antennae exist in two states, efficient in either energy transfer or energy dissipation, and in which those photosynthetic units in a dissipative state are unable to exchange energy with non-dissipative units.Abbreviations: F_o, F_m room-temperature chlorophyll fluorescence yield with all centres open, closed - F_v variable fluorescence yield - LHC II light-harvesting chlorophyll-protein complex of PS II - PS I, PS II Photosystem I, II - P700, P680 primary donor in Photosystem I, II - Q_A primary electron acceptor of PS II - P_max maximum quantum yield of oxygen evolution - qN coefficient of non-photochemical quenching of variable fluorescence - qN_e, qN_t, qN_i coefficient of non-photochemical quenching due to high-energy-state, state transition, photoinhibition - qO coefficient of quenching of dark level fluorescence - qP coefficient of photochemical quenching of variable fluorescence - _P intrinsic quantum yield of open PS II reaction centres = _s/qP - _{PS 2} quantum yield of PS = qP × F_v/F_m - _S quantum yield of oxygen evolution = rate of oxygen evolution/light intensity     

Photoinhibition of Photosystem I electron transfer activity in isolated Photosystem I preparations with different chlorophyll contents

Photoinhibition of the light-induced Photosystem I (PS I) electron transfer activity from the reduced dichlorophenol indophenol to methyl viologen was studied. PS I preparations with Chl/P700 ratios of about 180 (PS I-180), 100 (PS I-100) and 40 (PS I(HA)-40) were isolated from spinach thylakoid membranes by the treatments with Triton X-100, followed by sucrose density gradient centrifugation and hydroxylapatite column chromatography. White light irradiation (1.1 × 10⁴E m^–2 s^–1) of PS I-180 for 2 hours bleached 50% of the chlorophyll and caused a 58% decrease in the electron transfer activity with virtually no loss of the primary donor, P700. The flash-induced absorbance change showed the decay phase with a half time of about 10 s that was attributed to the P700 triplet, suggesting that the photoinhibitory light treatment caused the destruction of the PS I acceptor(s), F_x and possibly A₁. PS I-100 was similarly photobleached by the irradiation and the electron transfer activity decreased. There was, however, no apparent photoinhibition of the electron transport activity in PS I(HA)-40. Photoinhibition similar to that seen in PS I-180 also occurred in membrane fragments that were isolated without any detergent from a PS II-deficient mutant strain of the cyanobacterium Synechocystis sp. PCC 6803. PS I-180 was not photoinhibited under anaerobic conditions. The production of superoxide and fatty acid hydroperoxide during white light irradiation was significantly greater in PS I-180 than in PS I(HA)-40. The mechanism of photoinhibition in PS I preparations is discussed in relation to the formation of toxic oxygen molecules.Abbreviations A₀,A₁ primary and secondary electron acceptors of PS I - CD circular dichroism - DCPIP 2,6-dichlorophenol indophenol - F_A, F_B, F_X iron-sulfur centers A, B, X - HA hydroxylapatite - LHCI lightharvesting complex of PS I - MDA malondialdehyde - MV methyl viologen - Na-Asc sodium L-ascorbate - P700 primary electron donor of PS I - PFD photon flux density - PS I-A and PS I-B psaA and psaB gene products - TBA thiobarbituric acid