Energy transfers from Photosystem II to Photosystem I in Cryptomonas rufescens (Cryptophyceae)

In Cryptomonas rufescens (Cryptophyceae), phycoerythrin located in the thylakoid lumen is the major accessory pigment. Oxygen action spectra prove phycoerythrin to be efficient in trapping light energy.The fluorescence excitation spectra at ?196°C obtained by the method of Butler and Kitajima (Butler, W.L. and Kitajima, M. (1975) Biochim. Biophys. Acta 396, 72–85) indicate that like in Rhodophycease, chlorophyll a is the exclusive light-harvesting pigment for Photosystem I.For Photosystem II we can observe two types of antennae: (1) a light-harvesting chlorophyll complex connected to Photosystem II reaction centers, which transfers excitation energy to Photosystem I reaction centers when all the Photosystem II traps are closed. (2) A light-harvesting phycoerythrin complex, which transfers excitation energy exclusively to the Photosystem II reaction complexes responsible for fluorescence at 690 nm.We conclude that in Cryptophyceae, phycoerythrin is an efficient light-harvesting pigment, organized as an antenna connected to Photosystem II centers, antenna situated in the lumen of the thylakoid. However, we cannot afford to exclude that a few parts of phycobilin pigments could be connected to inactive chlorophylls fluorescing at 690 nm.     

Primary Events, Energy Transfer, and Reactions in Photosynthetic Units: Quantum Accumulation in Photosynthetic Oxygen Evolution

Three independent methods have been used to determine the size of the quantum accumulation unit in green plant photosynthesis. This unit is defined as that group of pigment molecules within which quantal absorption acts must take place leading to the evolution of a single O₂ molecule. All three methods take advantage of the nonlinearity of oxygen yield with light dose at very low dosages. The experimental values of this unit size, based on an assumed model for the charge cooperation in O₂ evolution, ranging from 800 to 1600, suggest that there is either limited energy transfer between energy-trapping units or chemical cooperation among oxygen precursors formed in several neighboring energy-trapping units. Widely diffusible essential precursors to molecular oxygen are ruled out by these results. Inhibition studies show that O₂ evolution is blocked when 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) is added to chloroplasts after two preliminary flashes and before a third flash which would have yielded O₂ in the absence of DCMU. This experiment is interpreted as evidence that the site of DCMU inhibition is on the oxidizing side of system II. Pretreatment of chloroplasts with large concentrations of Tris, previously believed to destroy O₂ evolution by blocking an essential reaction in the electron chain between water and system II, may be alternately interpreted as promoting the dark reversal of the system II light-induced electron transfer.     

New results on the properties of photosystem II centers blocked by 3-(3,4-dichlorophenyl)-1,1-dimethylurea in their different photoactive states

We have studied the 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) action on the different S states by oxygen, fluorescence and luminescence measurements.We show that no oxygen is evolved during a flash following the addition of DCMU to centers in their S₃ state. This suggests that oxygen inhibition cannot be attributed solely to a blocking between Q and A. For all the photoinactive states, the only remaining pathway for the quencher reoxidation, in the presence of DCMU, appears to proceed through a back reaction. Therefore, the complete quencher regeneration still occurring when the fourth positive charge is formed in the presence of DCMU is also an indication of an action by DCMU at the donor side.The data well fit the model in which the oscillations of the fluorescence yield and their damping are attributed to a fast equilibrium between two forms of the centers: a photoactive and a photoinactive form, both of which are quenchers. The equilibrium constant depends on the number of positive charges stored and DCMU changes the characteristics of this equilibrium.     

Energy and electron transfer in photosystem II of a chlorophyll b-containing Synechocystis sp. PCC 6803 mutant

Using a Synechocystis sp. PCC 6803 mutant strain that lacks photosystem (PS) I and that synthesizes chlorophyll (Chl) b, a pigment that is not naturally present in the wild-type cyanobacterium, the functional consequences of incorporation of this pigment into the PS II core complex were investigated. Despite substitution of up to 75% of the Chl a in the PS II core complex by Chl b, the modified PS II centers remained essentially functional and were able to oxidize water and reduce Q(A), even upon selective excitation of Chl b at 460 nm. Time-resolved fluorescence decay measurements upon Chl excitation showed a significant reduction in the amplitude of the 60-70 ps component of fluorescence decay in open Chl b-containing PS II centers. This may indicate slower energy transfer from the PS II core antenna to the reaction center pigments or slower energy trapping. Chl b and pheophytin b were present in isolated PS II reaction centers. Pheophytin b can be reversibly photoreduced, as evidenced from the absorption bleaching at approximately 440 and 650 nm upon illumination in the presence of dithionite. Upon excitation at 685 nm, transient absorption measurements using PS II particles showed some bleaching at 650 nm together with a major decrease in absorption around 678 nm. The 650 nm bleaching that developed within approximately 10 ps after the flash and then remained virtually unchanged for up to 1 ns was attributed to formation of reduced pheophytin b and oxidized Chl b in some PS II reaction centers. Chl b-containing PS II had a lower rate of charge recombination of Q(A)(-) with the donor side and a significantly decreased yield of delayed luminescence in the presence of DCMU. Taken together, the data suggest that Chl b and pheophytin b participate in electron-transfer reactions in PS II reaction centers of Chl b-containing mutant of Synechocystis without significant impairment of PS II function.     

Effects of carbonyl cyanide m-chlorophenylhydrazone and hydroxylamine on the Photosystem II electron exchange mechanism in 3-(3,4-dichlorophenyl)-1,1-dimethylurea treated algae and chloroplasts

The effects of NH₂OH and carbonyl cyanide m-chlorophenylhydrazone (CCCP) on 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU)-treated algae and chloroplasts were studied. In the presence of DCMU, the photochemically separated charges can only disappear through a recombination back reaction; both substances induce an irreversible reduction of the donor side and after sufficient illumination their action in the presence of DCMU leads to the formation of a permanent fluorescent state.

In the DCMU + CCCP system, a fast fluorescence induction curve is observed. The fluorescence yield is brought to its maximum by two flashes. The luminescence emission is strongly inhibited and most centers reach their permanent fluorescent state after one flash.

In the DCMU + NH₂OH system, a slow fluorescence rise is observed and several saturating flashes are needed for the fluorescence yield to reach its maximum. The exhaustion of the NH₂OH oxidizing capacity and the complete transformation to a permanent fluorescent state also require a large number of flashes.

The reduction pathway catalyzed by CCCP appears to be a good competitor to the back reaction, while NH₂OH seems to be a relatively inefficient donor.

In addition the action of NH₂OH and CCCP on fluorescence suggests that the donor side influences the quenching properties of Photosystem II centers. A possible mechanism is proposed.     

New results on the mode of action of 3,-(3,4-dichlorophenyl)-1,1-dimethylurea in spinach chloroplasts

Simultaneous measurements of hydroxylamine photo-oxidation and fluorescence induction were performed in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU). The results provide a justification for the common use of fluorescence data to estimate the concentration of active System II centers in the presence of inhibitors.The addition of DCMU to dark-adapted chloroplasts under special conditions induces a large increase of the initial yield of fluorescence. A reversible inactivation of part of the System II centers is responsible for this effect. Similar data were obtained with other classical inhibitors of oxygen evolution.     

UV-B induced alteration of oxygen evolving reactions in pea thylakoid membranes as affected by scavengers of reactive oxygen species

The effect of UV-B irradiation at temperatures of 22 and 4 °C on flash induced oxygen yields, photochemical activity, and energy transfer in pea thylakoid membranes in the absence and presence of scavengers of reactive oxygen species (ROS) was studied. Three different scavengers were used: dimethyl sulfoxide (DMSO), histidine (His), and n-propyl gallate (nPG). As result of the UV-B treatment of isolated membranes, the flash oxygen yields were considerably affected — the amplitudes decreased and the oscillation pattern was lost. The analysis of the flash oxygen yields and initial oxygen burst showed alterations of a number of oxygen evolving centers in the S0 state as well as changes of decay kinetics of the oxygen burst under continuous irradiation. ROS scavengers exhibited more or less expressed protective effects, nPG being the most effective against UV-B induced damages of the flash oxygen yields. At both the temperatures, photosystem II (PS II) mediated electron transport was more sensitive to the UV-B treatment in comparison with photosystem I (PS I). The analysis of 77 K fluorescence spectra showed that the fluorescence ratio F735/F685 increased by the UV-B treatment probably due to a redistribution of excitation energy between both photosystems most likely caused by partial unstacking and due to a decrease of PS II fluorescence resulting from reaction center-type quenching. The nPG was the most powerful scavenger which protected the oxygen evolution capacity of PS II in the absence and presence of an exogenous electron acceptor to the highest extent.     

Effective Absorption Cross-Sections in Porphyridium cruentum: Implications for Energy Transfer between Phycobilisomes and Photosystem II Reaction Centers

Effective absorption cross-sections for O₂ production by Porphyridium cruentum were measured at 546 and 596 nanometers. Although all photosystem II reaction centers are energetically coupled to phycobilisomes, any single phycobilisome acts as antenna for several photosystem II reaction centers. The cross-section measured in state I was 50% larger than that measured in state II.     

Energy transfer and quantum yield in Photosystem II

The photoreduction and dark reoxidation of Q_α and Q_β, the primary electron acceptors of Photosystems (PS) IIα and IIβ, respectively, in the presence of 3-(3′,4′-dichlorophenyl)-1,1-dimethylurea (DCMU) were studied in tobacco chloroplasts by means of fluorescence and absorbance measurements. The magnitude of a correction for an absorbance change by the oxidizing side of PS II needed in our previous study of the quantum yield of Q reduction (Biochim. Biophys. Acta 635 (1981), 111–120) has been determined. The absorbance change occurs in PS IIα mainly. The maximum fluorescence yield was found to be the same as in the mutant Su/su, which has a 3-fold higher reaction center concentration and a lower PS IIα to PS IIβ ratio. The kinetics of the light-induced fluorescence increase were measured after various pretreatments and the corresponding kinetics of the integrated fluorescence deficit were analyzed into their α and β components. From the results the contribution to the minimum fluorescence level, the degree of energy transfer between units, and the quantum efficiency of Q reduction were calculated for both types of PS II. This led to the following conclusions. The absence of energy between PS IIβ antennae is confirmed. Fluorescence quenching in PS IIα was adequately described by the matrix model, except for a decrease in the energy transfer between units during photoreduction of Q_α, possibly due to the formation of ‘islets’ of closed centers. PS II reaction centers in which Q is reduced do not significantly quench fluorescence. The ratio of variable to maximum fluorescence, 0.77 in PS IIα and 0.92 in PS IIβ, multiplied by the fraction of Q remaining in the reduced state after one saturating flash, 0.88 in PS IIα and greater than 0.95 in PS IIβ, leads to a net quantum efficiency of Q reduction in the presence of DCMU and NH₂OH of 0.68 in PS IIα and about 0.90 in PS IIβ. These values are in good agreement with the measured overall quantum efficiency of Q reduction.     

Light Energy Distribution in the Brown Alga Macrocystis pyrifera (Giant Kelp)

The brown alga Macrocystis pyrifera (giant kelp) was studied by a combination of fluorescence spectroscopy at 77 kelvin, room temperature modulated fluorimetry, and photoacoustic techniques to determine how light energy is partitioned between photosystems I and II in states 1 and 2. Preillumination with farred light induced the high fluorescence state (state 1) as determined by fluorescence emission spectra measured at 77K and preillumination with green light produced a low fluorescence state (state 2). Upon transition from state 1 to state 2, there was an almost parallel decrease of all of the fluorescence bands at 693, 705, and 750 nanometers and not the expected decrease of fluorescence of photosystem II and increase of fluorescence in photosystem I. The momentary level of room temperature fluorescence (fluorescence in the steady state, F_s), as well as the fluorescence levels corresponding to all closed (F_m) or all open (F_o) reaction-center states were measured following the kinetics of the transition between states 1 and 2. Calculation of the distribution of light 2 (540 nanometers) between the two photosystems was done assuming both the `separate package' and `spill-over' models. Unlike green plants, red algae, and cyanobacteria, the changes here of the light distribution were rather small in Macrocystis so that there was approximately an even distribution of the photosystem II light at 540 nanometers to photosystem I and photosystem II in both states 1 and 2. Photoacoustic measurements confirmed the conclusions reached as a result of fluorescence measurements, i.e. an almost equal distribution of light-2 quanta to both photosystems in each state. This conclusion was reached by analyzing the enhancement phenomenon by light 2 of the energy storage measured in far red light. The effect of light 1 in decreasing the energy storage measured in light 2 is also consistent with this conclusion. The photoacoustic experiments showed that there was a significant energy storage in light 1 which could be explained by cyclic electron transport around photosystem I. From a quantitative analysis of the enhancement effect of background light 2 (maximum enhancement of 1.4-1.5) it was shown that around 70% of light 1 was distributed to this cyclic photosystem I transport.     

Protection from photoinhibition by low temperature in Synechocystis 6714 and in Chlamydomonas reinhardtii: detection of an intermediary state

Photoinhibition was induced in a cyanobacterium strain, Synechocystis 6714, and a green alga, Chlamydomonas reinhardtii, by exposing them to light intensities from 1000 to 4000 microE/(m2.s) at various temperatures. The photoinhibition process was followed by measurements of chlorophyll fluorescence and oxygen evolution. During exposure to high light, fluorescent active reaction centers II became low fluorescent inactive centers. This process involved several reversible and irreversible steps. The pathway from the active state to the inactive low fluorescent state was different in Synechocystis and Chlamydomonas. In the latter there was a reversible intermediary step characterized by an increase of F0. This state was stable at 5 degrees C and slowly reversible at room temperature. The high F0 fluorescence level corresponded to a state of photosystem II centers that were inactive for oxygen evolution. An F0 decrease occurred in the dark in the absence of protein synthesis and was correlated to a restoration of oxygen evolution. Further experiments suggested that the existence of the intermediate fluorescent state is due to modified closed centers in which the reduced primary acceptor is less accessible to reoxidation. In cyanobacteria this reversible state was not detected. In both organisms, the decrease of Fmax reflected an irreversible damage of photosystem II centers. These centers need replacement of proteins in order to be active again. The quenching of Fmax and the irreversible inhibition of oxygen evolution were slowed down in both organisms by decreasing the temperature of the photoinhibitory treatment from 34 to 5 degrees C. We conclude that low temperature protected the reaction center II from irreversible photodamage.     

Photoinhibition in Chlamydomonas reinhardtii: Effect on state transition,intersystem energy distribution and Photosystem I cyclic electron flow

The energy distribution, state transitions and photosynthetic electron flow during photoinhibition of Chlamydomonas reinhardtii cells have been studied in vivo using photoacoustics and modulated fluorescence techniques. In cells exposed to 2500 W/m² light at 21 °C for 90 min, 90% of the oxygen evolution activity was lost while photochemical energy storage as expressed by the parameter photochemical loss (P.L.) at 710–720 nm was not impaired. The energy storage vs. modulation frequency profile indicated an endothermic step with a rate constant of 2.1 ms. The extent of the P.L. was not affected by DCMU but was greatly reduced by DBMIB. The regulatory mechanism of the state 1 to state 2 transition process was inactivated and the apparent light absorption cross section of photosystem II increased during the first 20 min of photoinhibition followed by a significant decrease relative to that of photosystem I. These results are consistent with the inactivation of the LHC II kinase and the presence of an active cyclic electron flow around photosystem I in photoinhibited cells.Abbreviations PS I, PS II Photosystem I and Photosystem II respectively - P.L. photochemical loss - DCMU 3-(3,4-dichlorophenyl-1,1-dimethyl urea - LHC II light harvesting chlorophyll a,b-protein complex of PS II - DBMIB 2,5 dibromo-3-methyl-6-isopropyl-p-benzoquinone     

Heat-induced changes of chlorophyll fluorescence in isolated chloroplasts and related heat-damage at the pigment level

The heat-induced changes of chlorophyll fluorescence excitation and emission properties were studied in isolated chloroplasts of Larrea divaricata Cav. An analysis of the temperature dependency of fluorescence, under Fo and Fmax conditions, of temperature-jump fluorescence induction kinetics, and of 77 degrees K emission spectra of preheated chloroplasts revealed two major components in the heat-induced fluorescence changes: (1) a fluorescence rise, reflecting the block of Photosystem II reaction centers; and (2) a fluorescence decrease, caused by the functional separation of light-harvesting pigment protein complex from the rest of the pigment system. Preferential excitation of chlorophyll a around 420 nm, produced a predominant fluorescence rise. Preferential excitation of chlorophyll b, at 480 nm, gives a predominant fluorescence decrease. It is proposed that the overlapping of the fluorescence decrease on the somewhat faster fluorescence rise, results in the biphasic fluorescence rise kinetics observed in isolated chloroplasts. Both the rise component and the decay component are affected by the thermal stability of the chloroplasts, acquired during growth of the plants in different thermal environments. Mg2+ enhances the stability against heat-damage expressed in the decrease component, but has no effect on the rise component. Heat pretreatment leads to a decrease of the variable fluorescence in the light-induced 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) rise curve, but no change in half-rise time is observed. It is concluded that the block of Photosystem II reaction centers precedes the loss of the light-harvesting pigment protein complex. However, the approximately antiparallel heat-induced Fmax decrease and Fo increase suggest a common cause for the two events. A heat-induced perturbation of the thylakoid membrane is discussed.     

Inhibition of O2 evolution by NADP in isolated potato tuber chloroplast and its identity with 3-(3,4-dichlorophenyl)-1,1-dimethyl urea inhibition site.

Chloroplast from greening potato tuber showed good photosynthetic capacity. The evolution of O₂ was dependent upon the intensity of light. A light intensity of 30 lux gave maximum O₂ evolution. At higher intensities inhibition was observed. The presence of bicarbonate in the reaction mixture was essential for O₂ evolution. NADP was found to be a potent inhibitor of O₂ evolution in this system. NADP and 3-(3,4-dichlorophenyl)-1,1-dimethyl urea (DCMU) inhibited the O₂ evolution completely at a 3 μm concentration level, which was reversed by oxidized 2,6-dichlorophenol-indophenol (DCIP). Cyanide (CN)-treated chloroplasts showed full O₂ evolution capacity, when a lipophilic electron acceptor like N-tetramethyl-p-phenylenediamine (TMPD) or DCIP was used along with ferricyanide. Ferricyanide alone showed only 20% reduction. NADP or DCMU could inhibit O₂ evolution only when TMPD was the acceptor but not with DCIP. Photosystem II (PS II) isolated from these chloroplasts also showed inhibition by NADP or DCMU and its reversal by DCIP. Here also the evolution of O₂ with only TMPD as acceptor was sensitive to NADP or DCMU. In the presence of added silicotungstate in PS II NADP or DCMU did not affect ferricyanide reduction or oxygen evolution. The chloroplasts were able to bind exogenously added NADP to the extent of 120 nmol/mg chlorophyll. It is concluded that the site of inhibition of NADP is the same as in DCMU, and it is between the DCIP and TMPD acceptor site in the electron transport from the quencher (Q) to plastoquinone (PQ).     

Functional Analysis of the Photosynthetic Apparatus of Prochlorothrix hollandica (Prochlorales), a Chlorophyll b Containing Procaryote

Light-shade adaptation of the chlorophyll a/b containing procaryote Prochlorothrix hollandica was studied in semicontinuous cultures adapted to 8, 80 and 200 μmole quanta per square meter per second. Chlorophyll a contents based on dry weight differed by a factor of 6 and chlorophyll b by a factor of 2.5 between the two extreme light conditions. Light utilization efficiencies determined from photosynthesis response curves were found to decrease in low light grown cultures due to lower light harvesting efficiencies; quantum requirements were constant at limiting and saturating irradiances for growth. At saturating growth irradiances, changes in light saturated oxygen evolution rate originated from changes in chlorophyll a antenna relative to the number of reaction centers II. At light-limiting conditions both the number of reaction centers II and the antenna size changed. The amount of chlorophyll b relative to reaction center II remained constant. As in cyanobacteria, the ratio of reaction center I to reaction center II was modulated during light-shade adaptation. On the other hand, time constants for photosynthetic electron transport (4 milliseconds) were low as observed in green algae and diatoms. The occurrence of state one to two and state two to one transitions is reported here. Another feature linking photosynthetic electron transport in P. hollandica to that in the eucaryotic photosynthetic apparatus was blockage of the state one to two transition by 3-(3,4-dichlorophenyl)-1,1-dimethylurea. Although chlorophyll b was reported in association with photosystem I, the 630 nanometer light effect does not exclude that chlorophyll b is the photoreceptor for the state one to two transition.     

Inactive Photosystem II Complexes in Leaves : Turnover Rate and Quantitation

The flash-induced electrochromic shift, measured by the amplitude of the rapid absorbance increase at 518 nanometers (ΔA518), was used to determine the amount of charge separation within photosystems II and I in spinach (Spinacia oleracea L.) leaves. The recovery time of the reaction centers was determined by comparing the amplitudes of ΔA518 induced by two flashes separated by a variable time interval. The recovery of the ΔA518 on the second flash revealed that 20% of the reaction centers exhibited a recovery half-time of 1.7 ± 0.3 seconds, which is 1000 times slower than normally active reaction centers. Measurements using isolated thylakoid membranes showed that photosystem I constituted 38% of the total number of reaction centers, and that the photosystem I reaction centers were nearly fully active, indicating that the slowly turning over reaction centers were due solely to photosystem II. The results demonstrate that in spinach leaves approximately 32% of the photosystem II complexes are effectively inactive, in that their contribution to energy conversion is negligible. Additional evidence for inactive photosystem II complexes in spinach leaves was provided by fluorescence induction measurements, used to monitor the oxidation kinetics of the primary quinone acceptor of photosystem II, Q_A, after a short flash. The measurements showed that in a fraction of the photosystem II complexes the oxidation of Q_A⁻ was slow, displaying a half-time of 1.5 ± 0.3 seconds. The kinetics of Q_A⁻ oxidation were virtually identical to the kinetics of the recovery of photosystem II determined from the electrochromic shift. The key difference between active and inactive photosystem II centers is that in the inactive centers the oxidation rate of Q_A⁻ is slow compared to active centers. Measurements of the electrochromic shift in detached leaves from several different species of plants revealed a significant fraction of slowly turning over reaction centers, raising the possibility that reaction centers that are inefficient in energy conversion may be a common feature in plants.     

Light Harvesting in Anacystis nidulans Studied in Pigment Mutants

Spontaneous pigment mutants of Anacystis nidulans were self-selected for improved growth in far red light (> 650 nanometers). Questions were asked about those features of the light-harvesting mechanism which altered to give the mutants improved photosynthetic performance in far red. Answers were sought by comparing pigment and reaction center concentrations for the parent and six mutants grown in gold fluorescent and in far red light. Three significant results emerged. The ratio of reaction centers for photoreactions I and II (RC1/RC2) varied by a value of about 2.1 for all clones grown in gold and a value of about 1.1 for all clones grown in far red. Alteration of the ratio was not evident in any of the mutants.     

Delayed fluorescence induction in chloroplasts. Irradiance dependence

We have studied the delayed fluorescence in spinach chloroplasts produced 0.5 ms after each of a pair of (sub)-microsecond flashes. We observe an increase in the delayed fluorescence from the second flash relative to that produced by the first. This increase is proportional to the product of the first and second flash irradiances, appearing as an I² dependence if both flashes are increased together. The enhancement is observable at very weak flash levels (roughly 1 photon absorbed/100 PS II centers). If the irradiance of the first flash is increased, but the irradiance of the second held constant, the delayed fluorescence from the second flash is observed to increase, but then to saturate well below the first flash irradiance at which the delayed fluorescence from the first flash itself saturates. For most experiments, the dark time between flashes was 30 ms. If the dark time is varied, the enhancement changes, reaching a half-maximal value for a dark time of approx. 300 μs. The enhancement is stopped by hydroxylamine, but not by gramicidin, valinomycin, DCMU, or mild heating. These experiments are consistent with the notion that there are two different types of Photosystem II centers if we assume that only one type is responsible for the induction we see and has an optical cross-section about 4-times the size of the other type of center.     

Flash-yield pattern for photosynthetic oxygen evolution in Chlorella and chloroplasts as a function of excitation intensity.

A study was carried out of the changes in flash-yield pattern for oxygen evolution at various light intensities. Oxygen measurements were made on algal and chloroplast samples, using a Joliot-type polarographic electrode. A mathematical model to describe the behavior of oxygen-evolving systems at various flash intensities was developed based on the binomial distribution. This model is capable of accurately predicting the oxygen flash-yield pattern over two orders of magnitude change in light intensity. The observed oxygen flash yields are accounted for at all flash intensities without changing the probability for misses and double hits by oxygen-evolving systems. It is concluded that intrinsic misses and double hits are observed, which are nearly independent of flash intensity. Also, the apparent optical cross section for oxygen evolution is found to increase as flash intensity decreases. It is suggested that inhomogeneity exists in the size of antenna-pigment aggregates associated with photosystem II reaction centers.     

Effects of 3-(3,4-Dichlorophenyl)-1,1-Dimethylurea on the Cell Cycle in Euglena gracilis

The cell cycle of the photosynthetic unicellular alga Euglena gracilis growing in phototrophic medium is regulated by light. To investigate the relationship of this cell cycle response to light stimulated photosynthesis, we have tested the effect of the photosynthesis inhibitor 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) on Euglena cell cycle transit. While DCMU does not block light stimulated cells from entering the S phase of the cell cycle, it does inhibit the transit through G₂/M. The specificity of this response and its relationship to photosynthesis was studied by looking at the effect of DCMU on dark grown wild-type cells, and on two bleached variants of Euglena (W₃BUL and W₁₀BSmL) that lack chloroplasts. The drug does block G₂/M in these cells, but not entrance into the cell cycle. Our studies show that entrance of cells into the cell cycle from a quiescent state does not require active photosynthesis, and that DCMU has effects on G₂/M transit that are independent of the photosynthetic capacity of the cells.