INACTIVATION OF THE ACCEPTOR SIDE AND DEGRADATION OF THE D1 PROTEIN OF PHOTOSYSTEM II BY SINGLET OXYGEN PHOTOGENERATED FROM THE OUTSIDE

Abstract— The possible association of photodynamic sensitization with photoinhibition damage to the photosystem II complex (PS II) has been investigated using isolated intact thylakoids from pea leaves. For this study singlet oxygen (¹O₂), photoproduced by endogenous chromophores that are independent of the function of PS II, was assumed to be the major reactive intermediate involved in the photoinhibition process. When thylakoid samples preincubated with rose bengal were subjected to exposure to relatively weak green light (500–600 nm) under aerobic conditions, PS II was severely damaged. The pattern of the rose bengal-sensitized inhibition of PS II was similar to that of high light-induced damage to PS II: (1) the secondary quinone (Q_B)-dependent electron transfer through PS II is inactivated much faster than the Q_B-independent electron flow, (2) PS II activity is lost prior to degradation of the D1 protein, (3) diuron, an herbicide that binds to the Q_B domain on the D1 protein, prevents D1 degradation, and (4) PS II is damaged to a greater extent by the deuteration of thylakoid suspensions but to a lesser extent by the presence of histidine. Furthermore, it was observed that destroying thylakoid Fe-S centers resulted in a marked reduction of high light-induced PS II damage. These results may suggest that the primary processes of photoinhibition are mediated by ¹O₂ and that Fe-S centers, which are located in some membrane components, but not in PS II, play an important role in photogenerating the activated oxygen immediately responsible for the initiation of photodamage to PS II.     

In situ SUSCEPTIBILITIES OF PHOTOSYSTEMS I AND II TO PHOTOSENSITIZED DEACTIVATION via SINGLET OXYGEN MECHANISM

Abstract— A comparative study was carried out on the in situ susceptibilities to photoinactivation of the photosystem I (PS I) and II (PS II) complexes of spinach thylakoids treated with efficient type II sensitizers. While the presence of the exogenous sensitizers caused a substantial increase in the extent of photoinactivation of whole chain electron transport, it did not affect PS I activity of thylakoids in light but exerted an enhanced photoinactivating effect only on PS II. The measurements of the action spectrum for the inhibition of PS II activity of the sensitizer-incorporated thylakoids and that for the generation of singlet oxygen (¹O₂) from them revealed that photosensitized inactivation of PS II is directly related to the photoproduction of ¹O₂ in thylakoid membranes. The results obtained in the present work clearly demonstrate an exceptional sensitivity of PS II to ¹O₂, providing circumstantial evidence that high light-induced damage to PS II may result from photosensitization reactions mediated by ¹O₂, which is not necessarily produced within the PS II complex.     

KINETIC STUDIES ON THE STABILIZATION OF THE PRIMARY RADICAL PAIR P680+ Pheo- IN DIFFERENT PHOTOSYSTEM II PREPARATIONS FROM HIGHER PLANTS*

Abstract— The stabilization of the primary radical pair P680+ pheophytin (Pheo)^- through rapid electron transfer from Pheo to the special plastoquinone of photosystem II (PS II), Q_A, was analyzed on the basis of time-resolved (40 ps) UV-absorption changes detected in different PS II preparations from higher plants. Lifetime measurements of¹Chi* fluorescence by single photon counting and a numerical analysis of the redox reactions revealed (1) at exciton densities required for light saturation of the stable charge separation, annihilation processes dominate the excited state decay leading to very similar lifetimes of ¹Chi* in systems with open and closed reaction centers and (2) the difference of absorption changes induced by actinic flashes of comparatively high photon density in samples with open and photochemically closed reaction centers, respectively, provides a suitable measure of the rate constant of QA formation. Conclusion 2 was confirmed in PS II membrane fragments by measurements at three wavelengths (280 nm, 292 nm and 325 nm) where the difference spectrum of Q^-_A formation exhibits characteristic features. The numerical evaluation of the experimental data led to the following results: (1) the rate constant of Q^-_A formation was found to be (300 ± 100 ps)^-1 in PS II membrane fragments and PS II core complexes deprived of the distal and proximal antenna and (2) an iron depletion treatment of membrane fragments does not affect these kinetics. The implications of these results are briefly discussed in terms of the PS II reaction pattern.     

STOICHIOMETRY and KINETICS OF PROTON RELEASE UPON PHOTOSYNTHETIC WATER OXIDATION

Abstract— We studied the magnitude and the rise kinetics of proton release into the interior of thylakoids by flash spectrophotometty with neutral red as pH indicator. Excitation of dark-adapted thylakoids by a series of between 4 and 11 flashes produced a complex pattern of proton release into the thylakoid lumen. Proton release upon each flash was time resolved.
A slow component of proton release oscillated weakly in magnitude with period of two as function of flash number. It exhibited a half-rise time of approximately 20 ms from the very first flash on, and it was abolished by inhibitors of plastohydroquinone oxidation. This component was attributed to the oxidation of plastohydroquinone by PS I via the Cytb₆/f complex.
Additionally, rapid and multiphasic proton release was observed with half-rise times of less than 2 ms which exhibited a pronounced and damped oscillation with period of four as function of flash number. This rapid proton release was attributed to water oxidation. A detailed kinetic analysis suggested that proton release occurred with the following stoichiometry and with the following half-rise times during the transitions S₁ S_i+1 of water oxidation: 1 H⁺(250 μs, S₀→₁): 0 H⁺(S₁→ S₂):1 H⁺(200 μs, S₂→S₃):2 H⁺(1.2 ms, S₃→ S₄→ S₀) . Proton release and proton rebinding upon oxidation and reduction of the intermediate electron carrier Z, respectively, may have influenced the kinetics of the respective proton yields but not the stoichiometric pattern.     

Amplified Degradation of Photosystem II D1 and D2 Proteins under a Mixture of Photosynthetically Active Radiation and UVB Radiation: Dependence on Redox Status of Photosystem II

Abstract— Plants exposed to a mixture of photosynthetically active radiation (PAR) and UVB radiation exhibit a marked boost in degradation of the D1 and D2 photosysteni II (PS II) reaction center proteins beyond that predicted by the sum of rates in PAR and UVB alone (amplified degradation). Becausee degradation driven by visible or UVB radiation alone is uncoupled from PS II redox status, it was therefore assumed that the mixed-light-amplified component of degradation would behave similarly. Surprisingly, amplified degradation proved to be coupled tightly to the redox status of PS II. We show that inactivation of the PS II water oxidation by heat shock or oxidation of the plastosemiquinone (Q_A-) by silicomolybdate nullifies only the amplified component of degradation but not the basic rates of degradation under PAR or UVB alone. The data are interpreted to indicate that formation of plastosemiquinone or an active water-oxidizing Mn₄ cluster, is the UVB chromophore involved in amplified degradation of the D1 and D2 proteins. Furthermore, accumulation of Q_A-by 3-(3,4-dichlorophenyl)-1,1-dimethylurea or 2-bromo-3-methyl-6-isopropyl-4-nitrophenol stimulated the mixed-light-amplified degradation component. Thus, amplified degradation of the D1 and D2 proteins in mixed radiance of PAR plus UVB (which simulates naturally occurring radiance) proceeds by a mechanism clearly distinct from that involved in degradation under PAR or UVB alone.     

LIGHT-INDUCED QUENCHING OF PHOTOSYSTEM II FLUORESCENCE AT 77 K

Abstract— Light-induced quenching of the low temperature fluorescence emission from photosystem II (PS II) at 695 nm ( F ₆₉₅) has been observed in chloroplasts and whole leaves of spinach. Photosystem I (PS I) fluorescence emission at 735 nm ( F ₇₃₅) is quenched to a lesser degree but this quenching is thought to originate from PS II and is manifest in a reduced amount of excitation energy available for spillover to PS I. Differential quenching of these two fluorescence emissions leads to an increase in the F ₇₃₅/ F ₆₈₅ ratio on exposure to light at 77 K. Rewarming the sample from -196°C discharges the thermoluminescence Z-band and much of the original unquenched fluorescence is recovered. The relationship between the thermoluminescence Z-band and the quenching of the low temperature fluorescence emission ( F ₆₉₅) is discussed with respect to the formation of reduced pheophytin in the PS II reaction center at 77 K.     

LASER PHOTOLYSIS OF 3-METHYLLUMIFLAVIN

Abstract— Using high-intensity actinic light, the chlorophyll a fluorescence transient from HCO^-₃-depleted chloroplasts shows a rapid initial rise (O → I) followed by a slow phase (I → P). In the presence of HCO^-₃, the O → I rise is delayed but the I → P phase is much more rapid. Using low-intensity actinic light, the chlorophyll a fluorescence transient from 3-(3,4-dichlorophenyl)-1,1 dimethylurea (DCMU)-treated chloroplasts is delayed in the presence of HCO^-₃. Bicarbonate increases the amount of delayed light emission from chloroplasts given 10 s illumination with weak blue light (0·4 W/m²). DCMU greatly increases the amount of delayed light seen in the presence of HCO^-₃ under these conditions but decreases the amount seen in the absence of HCO^-₃. It is suggested that HCO^-₃ may somehow form or stabilize, in the dark, a number of reaction centers corresponding to the S₁ state in the model of B. Forbush, B. Kok and M. McGloin ( Photochem. Photobiol. 14, 307–321, 1971).     

THE LIGHT DEPENDENT QUENCHING OF CHLOROPLAST FLUORESCENCE BY COFACTORS OF CYCLIC ELECTRON FLOW IN PHOTOSYSTEM I

Abstract—When 3–(3',4'-dichlorophenyl)-1,1-dimethylurea poisoned, intact thylakoids of isolated chloroplasts are illuminated in salt free suspension media, N -methylphenazinium cations (MP⁺) are reversibly taken up. Simultaneously, the chlorophyll fluorescence is reversibly lowered. When inorganic salts in the reaction medium provide membrane permeant charge balancing ions, the extent of the MP⁺ association with the thylakoids is strongly increased, but the fluorescence lowering is hardly affected. lonophoretically active agents inhibit specifically the salt dependent increment of the MP⁺ interaction with the thylakoids, but have only insignificant effects on the fluorescence lowering provided the experimental conditions do not allow the formation of a proton gradient across the thylakoid membrane. On the basis of these results, and of data obtained from comparative studies with other cofactors of cyclic electron transport in PS I, it is suggested that the 'energy dependent' fluorescence lowering is linked to a binding of cationic cofactors to nucleophilic sites in or at the thylakoid membrane. Such sites appear to become exposed in the wake of a light dependent transport of the cofactor, or of protons, into the thylakoid.     

MULTIPLE ACTION OF FAR-RED LIGHT IN PHOTOPERIODIC INDUCTION and CIRCADIAN RHYTHMICITY

Abstract— It is generally accepted that phytochrome influences the photoperiodic induction of flowering through its interaction with the circadian clock mechanism. We have attempted to separate the effects of phytochrome on the clock mechanism from those that mediate flowering directly by examining a number of responses that are unrelated to flowering but are also regulated by the circadian clock. Gas exchange measurements of both CO₂ and H₂0 vapor were monitored under light conditions (200 μmol m ² s⁻¹) where the addition of far-red energy is required for the maximal promotion of flowering. In addition, photosynthetic capacity and maximal transpiration rates were measured in plants grown under continuous dim (20 μmol m⁻² S⁻') light, with or without supplemental far-red, by exposing them briefly to saturating fluxes (1000 μmol m⁻² s^-l) of light. Net CO₂ fixation was very weakly rhythmic in plants grown under both high and low light and this weak oscillation was completely suppressed by far-red light. Far-red also suppressed the rhythm in transpiration under high light, but the rhythm was immediately reinstated when the far-red light was removed. The phase of this rhythm was also reset with the next peak always occurring15–18 h after the far-red was turned off. When grown under dim light, the transpiration rhythm was not suppressed and the amplitude of the oscillation was more than doubled. Far-red light appears to interact with the rhythm in transpiration in a manner suggesting that the stomatal rhythm may be coupled to the same clock oscillator that regulates the flowering rhythm.     

TEMPERATURE DEPENDENCE OF DELAYED LIGHT EMISSION IN THE 6 to 340 MICROSECOND RANGE AFTER A SINGLE FLASH IN CHLOROPLASTS

Abstract. The delayed light emission decay rate (up to 120 μs) and the rise in chlorophyll a fluorescence yield (from 3 to 35 μs) in isolated chloroplasts from several species, following a saturating 10 ns flash, are temperature independent in the 0–35°C range. However, delayed light in the 120–340 μs range is temperature dependent. Arrhenius plots of the exponential decay constants are: (a) linear for lettuce and pea chloroplasts but discontinuous for bush bean (12–17°C) and spinach (12–20°C) chloroplasts; (b) unaffected by 3-(3,4 dichlorophenyl)-1,1-dimethylurea (inhibitor of electron flow), gramicidin D (which eliminates light-induced membrane potential) and glutaraldehyde fixation (which stops gross structural changes).
The discontinuities, noted above for bush bean and spinach chloroplasts, are correlated with abrupt changes in (a) the thylakoid membrane lipid fluidity (monitored by EPR spectra of 12 nixtroxide stearate, 12NS) and (b) the fluidity of extracted lipids (monitored by differential calorimetry and EPR spectra of 12 NS). However, no such discontinuity was observed in (a) chlorophyll a fluorescence intensity of thylakoids and (b) fluorescence of tryptophan residues of delipidated chloroplasts.
Microsecond delayed light is linearly dependent on light intensity at flash intensities as low as one quantum per 2 times 10⁴ chlorophyll molecules. We suggest that this delayed light could originate from a one quantum process in agreement with the hypothesis that recombination of primary charges leads to this light emission. A working hypothesis for the energy levels of Photosystem II components is proposed involving a charge stabilization step on the primary acceptor side, which is in a lipid environment.
Finally, the redox potential of P680 (the reaction center for chlorophyll of system II) is calculated to be close to 1.0–1.3 V.     

THE PHOTOBIOLOGY OF Paphiopedilum STOMATA: OPENING UNDER BLUE BUT NOT RED LIGHT

Abstract— The responses of stomata from Paphiopedilum harrisianum , Orchidaceae, to light and CO₂ were studied in epidermal peels. Stomatal opening under red light was indistinguishable from that in darkness, whereas blue light promoted opening above dark levels. The ineffectiveness of red light in causing stomatal opening was confirmed in the presence of 100 μ M KCN; average apertures in both darkness and red light were 53% of those measured in the absence of the inhibitor, whereas under blue irradiation, the KCN inhibition was only 30%, with average apertures two-fold of those measured under red light or darkness. Fluence rate response curves under blue light were typical of a single photoreceptor; removal of CO₂ increased aperture values without a significant light-CO₂ interaction. The lack of a stomatal red light response contrasts with results obtained in species with chlorophyllous stomata in which red light consistently causes stomatal opening, and suggests that the previously reported red light responses in stomata from intact Paphiopedilum leaves resulted from indirect effects, such as depletion of intercellular CO₂ by mesophyll photosynthesis. In isolation, Paphiopedilum stomata appear to rely on a blue light photosystem for their responses to light and fail to open under red light because of their lack of guard cell chloroplasts.     

PHOTOCONVERSION OF PHYTOCHROME IN VIVO STUDIED BY DOUBLE FLASH IRRADIATION IN Mougeotia AND Avena

Abstract— The kinetics of phytochrome phototransformation from the red-absorbing form (P_r) to the far-red-absorbing form (P_fr) in vivo at 22°C were studied using a double flash apparatus with 1-ms flashes. Photoconversion by simultaneous flashes of red light saturates at a low P_fr level, indicating the possible attainment of a photoequilibrium between the excitation of P_r and the photoreversion of intermediates in the course of the I-ms flashes. At saturation energy, simultaneous flashes resulted in about 50% as much P_fr as was produced by saturating irradiation with 5 s red light. Intermediates of the phototransformation pathway were analysed by separating two red or a red and a far-red flash by variable dark intervals. In both plants phototransformation intermediates with half-lives < 1 ms occur, but they are too short-lived to characterize by our method. The subsequent intermediates have half-lives of about 7 ms and 150 ms in A vena , 2 ms and 10 ms in Mougeotia. The conversion from P_r to P_fr seems to be completed 1 s after the red flash in Avena. In the alga Mougeotia , P_fr formation seems to be finished within only 50 ms after the inducing red flash. The kinetics obtained from physiological and spectrophotometric experiments with Avena mesocotyls are almost identical. These observations indicate that the physiological response corresponds directly to the amount of P_fr produced and not to phototransformation intermediates or "cycling" between P_r and P_fr.     

DETERMINATION OF THE KINETICS OF THE BACK REACTION OF PHOTOSYSTEM II IN THE PRESENCE OF 3–(3,4-DICHLORPHENYL)-1,1-DIMETHYLUREA FROM LUMINESCENCE MEASUREMENTS

Abstract— An alternative method to that used by Mar and Roy (1974) for the determination of the kinetics of the back reaction of photosystem II from the luminescence decay curve in the presence of 3–(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) has been suggested. The new theory relies upon two hypotheses: the well-known recombination hypothesis of luminescence and the assumption that the luminescence yield in the seconds region is given by the variable part of the live fluorescence yield. The second hypothesis was introduced since assuming a constant luminescence yield results in kinetic data that are not consistent with measurements of the kinetics of the back reaction by the restoration of the area over the fluorescence rise curve. The dependence of the live fluorescence yield from the concentration of closed PS II traps was assumed to be represented by Delosme's expression originally derived for the rise curve of the fluorescence yield in the presence of DCMU.
The theory is based on the fact that then the partial and total light sums of luminescence are simple functions of the concentration of the primary electron acceptor Q^- of PS II. Thus, after integrating the luminescence decay curve the theory permits a convenient evaluation of the kinetics of the back reaction [Q^-]( t ) in terms of the partial and total light sum.
This method was applied in order to determine the kinetics of the back reaction in Chlorella fusca in the presence of DCMU. It is shown that the kinetics of deactivation of the S, state can be described using the expression for the kinetics of the back reaction derived by Mar and Roy. As an alternative explanation, a biphasic first order decay of S₂ is proposed.     

COPPER QUENCHING OF THE VARIABLE FLUORESCENCE IN Dunaliella tertiolecta. NEW EVIDENCE FOR A COPPER INHIBITION EFFECT ON PSII PHOTOCHEMISTRY

Abstract— The copper quenching effect on fluorescence in Dunaliella tertiolecta was studied. 30% of variable fluorescence was quenched in the presence of 70 μ,M CuS0₄. We confirmed that the copper inhibitory effect on photosystem II (PSII) activity is located on its oxidizing side. Further, we indicate that the complementary area is decreased by copper. Since the quantum yield of PSII photochemistry was lowered and the rate of PSII primary electron acceptor Q_A remained unaffected, we can conclude that some PSII reaction centers were inactivated by copper.     

A LASER FLASH PHOTOLYSIS STUDY OF PYRENE-1-ALDEHYDE. INTERSYSTEM CROSSING EFFICIENCY, PHOTOREACTIVITY AND TRIPLET STATE PROPERTIES IN VARIOUS SOLVENTS

Abstract— Triplet-and singlet-related photoprocesses of pyrene-1-aldehyde (PA) in various solvents have been investigated in detail using 337.1 and 355 nm laser flash photolysis in conjunction with time-correlated determination of fluorescence lifetimes (τ_F) and steady-state photochemical and absorption-emission spectral measurements. In benzene, the lowest triplet of PA (43 < E_T < 46 kcal/mol) has a lifetime of about 50 µs (τ_T) and displays the absorption maximum at 443 nm with a maximum extinction coefficient (ε_max) of 21000 M ^-1cm^-1; the corresponding ketyl radical has a sharp absorption maximum at 428 nm (ε_max≥ 25000 M ^-1cm^-1). The quantum yields (φ_T) of lowest triplet occupation are high in nonprotic solvents (0.6–0.8), decrease in protic solvents (alcohols) as the polarity of the latter is increased, and maintain a complementary relationship with the quantum yields (φ_F) of fluorescence. Quantum yields (φ_PC) of loss of PA due to photoreactions in some solvents have also been determined under conditions of steady irradiation at 366 nm; φ_PC is in the range 0.1–0.2 in electron-rich olefinic solvents such as cyclohexene and tetramethylethylene. These results concerning τ_F, τ_T, φ_F. φ_T and φ_PC as well as the effects of 1,2,4-trimethoxybenzene and 2,5-dimethyl-2,4-hexadiene as quenchers for fluorescence, triplet yield, and photochemistry are discussed in the light of possible state orders for PA in polar and nonpolar environments.     

THE SUSCEPTIBILITY OF MUNG BEAN CHLOROPLASTS TO PHOTOINHIBITION IS INCREASED BY AN EXCESS SUPPLY OF IRON TO PLANTS: A PHOTOBIOLOGICAL ASPECT OF IRON TOXICITY IN PLANT LEAVES

In an attempt to elucidate the underlying mechanisms for iron toxicity in plants, the combined effects of iron overload and light intensities on the photosynthetic capacity of leaves were particularly focussed upon in this study, using mung bean seedlings grown under varied conditions regarding the supply of light and iron. The seedlings, when supplied with excess iron (up to 1.0 m M ) and low light (40 W/m²), did not suffer any loss of photosynthesis; further, the typical symptoms of iron toxicity, as shown in the leaves grown in sunlight at ca 450 W/m² on an average, were not seen in those. Nonetheless, excess iron supply resulted in a marked increase in photosensitivity of the low light-adapted seedlings. A large portion of iron accumulated in chloroplasts by the supply of excess iron was found to be incorporated into thylakoids as nonheme iron (NHI), which acts as a potent sensitizer, photogenerating singlet oxygen (¹O₂). The generation rate of ¹O₂ from thylakoids linearly increased with increasing content of NHI; this was in parallel with the NHI content dependence of photoinactivation rates of photosynthetic electron transport and key enzymes of the Calvin cycle in chloroplasts. The results suggest that Fe-dependent photosensitization reactions, occurring via the ¹O₂ mechanism, may be deeply involved in cellular processes leading to developing iron toxicity symptoms in plants.     

ESTIMATION OF ENERGY DISTRIBUTION AND REDISTRIBUTION AMONG TWO PHOTOSYSTEMS USING PARALLEL MEASUREMENTS OF FLUORESCENCE LIFETIMES AND TRANSIENTS AT 77 K

Abstract— A single-sample method for estimating energy distribution and redistribution among the two photosystems using fluorescence lifetimes and transients at 77 K is presented. In this method,α(the fraction of photons absorbed by photosystem I, PSI) is F_1(α)/(F_1(α)+ (τ_{F 1(M)}/τ_{F 2(M)}).F_2(M)) where, F_1(α) is the fluorescence intensity from PSI excited by photons initially absorbed by the latter, τ_{F 1(M)} and τ_{F 2(M)} are the maximum lifetimes of fluorescence from chlorophyll- a in PSI (1) and II (2), and, F_2(M) is the maximum fluorescence intensity from PSII (P level). Analysis of the intensities and lifetimes of wavelength resolved fluorescence of thylakoids (pH 7.0), with and without cations, leads to the following conclusions: The addition of 10 m M Na⁺ to cation-depleted thylakoids (pH 7.0) increases α by ˜ 10%, while the subsequent addition of 10 m M Mg²⁺ leads to three principal concomitant changes (in the order of importance): a 50% decrease in PSII to PSI energy transfer, a 20% increase in other radiation-less losses, and a 10% decrease in α.     

Modulation of photosystem II chlorophyll fluorescence by electrogenic events generated by photosystem I.

In an attempt to uncover electric field interactions between PS I and PS II during their functioning, fluorescence induction curves were measured on hydroxylamine-treated thylakoids of Chenopodium album under conditions ensuring low and high levels of photogenerated membrane potentials. In parallel experiments with Peperomia metallica chloroplasts, the photocurrents were measured with patch-clamp electrodes and served as indicator of electrogenic activity of thylakoid membranes in continuous light. Inhibition of linear electron flow at PS II donor side by hydroxylamine (0.1 mM) eliminated a slow rise of chlorophyll fluorescence to a peak level and suppressed photoelectrogenesis. Activation of PS I-dependent electron transport using cofactors of either cyclic (phenazine methosulfate) or noncyclic electron transport (reduced TMPD or DCPIP in combination with methyl viologen) restored photoelectrogenesis in hydroxylamine-treated chloroplasts and led to reappearance of slow components in the fluorescence induction curve. Exposure of thylakoids to valinomycin reduced the peak fluorescence in the presence of KCl but not in the absence of KCl. Combined application of valinomycin and nigericin in the presence of KCl exerted stronger suppression of fluorescence than valinomycin alone but was ineffective in the absence of KCl. In samples treated with hydroxylamine and PS I cofactors (DCPIP/ascorbate and methyl viologen), preillumination with a single-turnover flash or a multiturnover pulse shifted the induction curves of both membrane potential and chlorophyll fluorescence to shorter times, which confirms the supposed influence of PS I-generated electrical field on PS II fluorescence. A model is presented that describes modulating effect of the membrane potential on chlorophyll fluorescence and roughly simulates the fluorescence induction curves measured at low and high membrane potentials.     

GENETIC VARIATIONS AND LINOLENIC ACID INDUCED CHANGES IN THE ORIENTATION PATTERN OF CHLOROPHYLL a IN THYLAKOID MEMBRANES

Abstract Orientation pattern of the Q_y absorption and emission dipoles of chlorophyll a were studied in wild type Scenedesmus obliquus and in mutants deficient in chlorophyll b and carotenoids. Fluorescence polarization ratio at –140°C and linear dichroism at 25°C were measured in whole cells and thylakoids aligned in polyacrylamide gel. Unlike normal thylakoids, mutants displayed fluorescence polarization ratios significantly lower than 1.0 and showed a negative LD signal around 672 nm, indicating the tendency of the Q_y dipoles to tilt out from the membrane plane. Such an orientation pattern can also be artificially induced by treating normal thylakoids with linolenic acid.     

PHOTOCHEMISTRY OF RETINOCHROME

Abstract— Retinochrome is a photopigment found in the visual cells of cephalopods. It has been considered to act as a supplier of the 11- cis -retinal required for synthesis of rhodopsin, because its all-trans chromophore is isomerized to 11- cis form in the light. Light and thermal reactions of squid retinochrome were investigated by low-temperature spectrophotometry.
On irradiation with green light at liquid-nitrogen temperature, retinochrome (λ_max 496 nm, – 190°C) is converted mainly to an intermediate lumiretinochrome (λ_max 475 nm, – 190°C), its chromophore being changed to 11- cis -retinal. On irradiation with blue light at - 190°C, retinochrome is changed to a photosteady–state mixture (λ_max 487 nm, – 190°C) composed mainly of retinochrome and lumiretinochrome, since lumiretinochrome is partially regenerated back to retinochrome. Similarly, irradiation of lumiretinochrome with blue light also results in the same photosteady-state mixture, which can be completely reverted to lumiretinochrome on re-irradiation with green light.
Lumiretinochrome is stable at a wide range of temperatures from – 190°C to about – 20°C. Above – 20°C, it is further converted, thermally, into metaretinochrome (λ_max 470 nm), which is the same bleached product as has been observed on irradiation of retinochrome at room temperatures. Thus, the light-bleaching process of retinochrome is rather simple compared with that of rhodopsin.