Two effects of electrical fields on chloroplasts

An electrical field across a suspension of Chenopodium chloroplasts stimulates the emission of delayed light during the time the field is on. This stimulation can be used to calculate the distance over which the electron moves in the untrapping process that gives the delayed light. An electrical field applied at the time of illumination gives a polarization to the suspension of chloroplasts that lasts for some seconds. This polarization is a new way to study delayed light and fluorescence from chloroplasts.     

Characteristics of Prompt and Delayed Fluorescence from Spinach Chloroplasts

Effects of ferricyanide, dichlorophenyldimethylurea (DCMU), and uncouplers of phosphorylation on the prompt and delayed fluorescences from spinach chloroplasts are described. Any factor that affects the yield of prompt fluorescence will similarly influence the intensity of delayed fluorescence. This idea, recently investigated by Lavorel, should be expressed in terms of a “live” component of fluorescence; that is, the component from chlorophyll associated with the photochemical traps of System II. Some of the effects of ferricyanide and DCMU on delayed fluorescence can then be explained in terms of effects on the yield of prompt fluorescence. From the internal consistency of the explanation, applied to various observations, a judgment can be made that most of the prompt fluorescence observed initially when dark-adapted chloroplasts are first illuminated is “dead,” coming from chlorophyll not associated with trap II. The live fluorescence is represented almost entirely by the time-varying component that develops during illumination. The observed intensity of delayed fluorescence can be divided by the yield of live prompt fluorescence to give an intrinsic delayed fluorescence. This intrinsic delayed fluorescence is proportional to the square root of exciting light intensity (as long as the excitation is not saturating) and decays with second order kinetics. This behavior may reflect the photochemical formation and second order dissipation of an oxidized product of Photosystem II.     

Primary Events, Energy Transfer, and Reactions in Photosynthetic Units: A Connected Model of the Photosynthetic Unit

The concept of photosynthetic unit (PSU) is reviewed in the light of the authors' results in the fields of fluorescence and luminescence (delayed light). Models of PSU are mainly distinguished by the amount of exciton exchange which is allowed between units. The “separate” model, with its “first-order” character, is not consistent with fluorescence kinetic data. The sigmoidal rise of fluorescence under actinic light is best explained by “nonseparate” models; however, most of these models assume a delocalization of excitons or centers. The “connected” model introduced here is not subject to this criticism. It discloses a new effect (the “îlot” effect): a nonrandom grouping of fluorescent units the consequences of which are discussed. It is noted that a “two-quantum” model for the photochemical reaction gives results very similar to those of the connected model. A relation between luminescence intensity and fluorescence yield is seen as a necessary consequence of the PSU concept. Its meaning is different in separate and nonseparate models. This relation is discussed in connection with the true system II fluorescence emission.     

External electric field effects on prompt and delayed fluorescence in chloroplasts

An electric field pulse was applied to a suspension of osmotically swollen spinach chloroplasts after illumination with a saturating flash in the presence of DCMU. In addition to the stimulation of delayed fluorescence by the electric field, discovered by Arnold and Azzi (Arnold, W.A. and Azzi, R. (1971) Photochem. Photobiol. 14, 233–240) a sudden drop in fluorescence yield was observed. The kinetics of this fluorescence change were identical to those of the integrated delayed fluorescence emission induced by the pulse. The S-state dependence of the stimulated emission was very similar to that of the normal luminescence. We assume that the membrane potential generated by the pulse changes the activation energy for the back reaction in Photosystem II. On this basis, and making use of data we obtained earlier from electrochromic absorbance changes induced by the pulse, the kinetics of the field-induced prompt and delayed fluorescence changes, and also the amplitude of the fluorescence decrease, which was about 12% for a nearly saturating pulse, are explained. Our results indicate that in those reaction centers where a decrease of the activation energy occurs the effect of a pulse can be quite spectacular: the back reaction, which normally takes seconds, is completed in a few hundred microseconds when a sufficiently strong pulse is applied. Measurements of the polarization of the stimulated luminescence supported the interpretation given above.Only 2.8% of the back reaction was found to proceed via transition of reexcited chlorophyll to the ground state, both during the field pulse and in the absence of the field.     

Characteristics of Fluorescence and Delayed Light Emission from Green Photosynthetic Bacteria and Algae

Green photosynthetic bacteria exhibit variations in the intensity of their fluorescence during illumination. The initial intensity of fluorescence, measured at the onset of illumination, has a spectrum in which the major pigment Chlorobium chlorophyll predominates. The minor pigment bacteriochlorophyll predominates in the spectrum of the time-varying part of the fluorescence. The spectrum of delayed light emission is identical to that of the time-varying fluorescence. The variations in fluorescence also resemble the delayed light in their kinetics and in their dependence on exciting light intensity. Similar results are obtained for the kinetics of prompt and delayed light emission in the algae Chlorella and Anacystis. These findings raise the possibility that the variations in fluorescence actually represent a fast component of delayed light emission, of intensity comparable to the intensity of fluorescence. In Anacystis there is an outburst of light emission that develops after the exciting light has been turned off, reaching a maximum intensity after 1 to 3 seconds. This emitted light has the spectrum of chlorophyll fluorescence. It appears to be a novel example of bioluminescence with singlet excited chlorophyll as the emitter.     

Further characterization of a photosystem ii particle isolated from spinach chloroplasts by triton treatment delayed light emission

Delayed light emission from the Triton-fractionated Photosystem II subchloroplast fragments (TSF-IIa) was measured between 0.5 and 10 ms after the termination of illumination. The delayed light emission was diminished by Photosystem II inhibitors, DCMU and o-phenanthroline, which act between the reduced primary acceptor and the plastoquinone pool.Secondary electron donors to Photosystem II, diphenylcarbazide, phenylenediamine, Mn²⁺, and ascorbate inhibited delayed light emission. Secondary electron acceptors such as ferricyanide, dichlorophenol indophenol, and dimethyl benzoquinone enhanced delayed light emission. The addition of secondary electron acceptors to TSF-IIa particles containing Mn²⁺ restored delayed light emission to almost the control level. The plastoquinone antagonist, 2,5-dibromo-3-methyl-6-isopropyl p-benzoquinone, increased delayed light emission at low concentrations but decreased it at higher concentrations. Silicomolybdate enhanced the delayed light emission of TSF-IIa particles markedly, and reversed the inhibition by DCMU. Silicomolybdate showed a similar stimulatory effect on the delayed-light intensity in broken spinach chloroplasts at shorter times after the termination of illumination. Carbonyl cyanide m-chloro (or p-trifluoromethoxy) phenylhydrazones inhibited the delayed light emission, but NH₄Cl had no effect.     

Delayed light studies on photosynthetic energy conversion. VII. Effect of the high energy state, coupled to 2,3,5,6-tetramethyl p-phenylenediamine-catalyzed cyclic electron flow, on millisecond emission from chloroplasts and digitonin subchloroplast particles

The effect of 2,3,5,6-tetramethyl p-phenylenediamine-catalyzed cyclic electron flow on millisecond delayed light emission from chloroplasts has been compared to the effect on subchloroplast particles. Non-cyclic electron flow of both chloroplasts and subchloroplast particles was blocked with 3-(3,4-dichlorophenyl)-1,1-dimethylurea. 2,3,5,6-tetramethyl p-phenylenediamine-catalyzed cyclic electron flow increased the millisecond delayed emission by 2–4 times in both chloroplasts and subchloroplast particles. Uncoupling conditions which collapse only the pH gradient component of the proton motive force reduced the 2,3,5,6-tetramethyl p-phenylenediamine stimulation of delayed light in chloroplasts but not in particles. The 2,3,5,6-tetramethyl p-phenylenediamine stimulation of delayed light in particles was sensitive to uncoupling conditions which are presumed to destroy the transmembrane potential. Energy transfer inhibitors were without effect on the 2,3,5,6-tetramethyl p-phenylenediamine stimulation in both chloroplasts and particles.

The 2,3,5,6-tetramethyl p-phenylenediamine stimulation of millisecond delayed emission appears to reflect the particular form of the proton motive force; in chloroplasts it seems to be correlated with the proton concentration gradient, whereas in particles it is more closely correlated with the transmembrane potential.     

The coleoptile chloroplast: Distinct distribution of xanthophyll cycle pigments,and enrichment in Photosystem II

Recent studies have shown that coleoptile chloroplasts operate the xanthophyll cycle, and that their zeaxanthin concentration co-varies with their sensitivity to blue light. The present study characterized the distribution of photosynthetic pigments in thylakoid pigment–protein complexes from dark-adapted and light-treated coleoptile and mesophyll chloroplasts, the low temperature fluorescence emission spectra, and the rates of PS I and PS II electron transport in both types of chloroplasts from 5-day-old corn seedlings. Pigments were extracted from isolated PS I holocomplex, LHC IIb trimeric and LHC II monomeric complexes and analyzed by HPLC. Chlorophyll distribution in coleoptile thylakoids showed 31% of the total collected Chl in PS I and 65% in the light harvesting complexes of PS II. In mesophyll thylakoids, the values were 44% and 54%, respectively. Mesophyll and coleoptile PS I holocomplexes differed in their Chl t a/Chl t b ratios (8.1 and 6.1, respectively) and -carotene content. In contrast, mesophyll and coleoptile LHC IIb trimers and LHC II monomers had similar Chl t a/Chl t b ratios and -carotene content. The three analyzed pigment–protein complexes from dark-adapted coleoptile chloroplasts contained zeaxanthin, whereas there was no detectable zeaxanthin in the complexes from dark-adapted mesophyll chloroplasts. In both chloroplast types, zeaxanthin and antheraxanthin increased markedly in the three pigment–protein complexes upon illumination, while violaxanthin decreased. In mesophyll thylakoids, zeaxanthin distribution as a percentage of the xanthophyll cycle pool was: LHC II monomers > LHC IIb trimers > PS I holocomplex, and in coleoptile thylakoids, it was: LHC IIb trimers > LHC II monomers = PS I holocomplex. Low temperature (77 K) fluorescence emission spectra showed that the 686 nm emission of coleoptile chloroplasts was approximately 50% larger than that of mesophyll chloroplasts when normalized at 734 nm. The pigment and fluorescence analysis data suggest that there is relatively more PS II per PS I and more LHC I per CC I in coleoptile chloroplasts than in mesophyll chloroplasts. Measurements of t in vitro uncoupled photosynthetic electron transport showed approximately 60% higher rates of electron flow through PS II in coleoptile chloroplasts than in mesophyll chloroplasts. Electron transport rates through PS I were similar in both chloroplast types. Thus, when compared to mesophyll chloroplasts, coleoptile chloroplasts have a distinct PS I pigment composition, a distinct chlorophyll distribution between PS I and PS II, a distinct zeaxanthin percentage distribution among thylakoid pigment–protein complexes, a higher PS II-related fluorescence emission, and higher PS II electron transport capacity. These characteristics may be associated with a sensory transducing role of coleoptile chloroplasts.     

The Influence of Two Naturally Occurring Factors, from the Leaves of Ricinus Communis, on the Fluorescence Induction of Higher Plant Chloroplasts and Intact Algae

Changes in fluorescence induction, brought about by incubation of chloroplasts (Zea mays) in an aqueous extract of Ricinus leaf, have been divided, on the basis of speed of manifestation, into two categories: “fast” changes and “slow” changes (i.e. those observed after 5 min and 1½ hr of incubation, respectively). The former, which include a large increase in the magnitude of the fast component of variable fluorescence and a retardation of decay from maximum to minimum levels of fluorescence, have been ascribed to inhibition of electron transport at a site beyond that of 3-(p-chlorophenyl)-1,1-dimethylurea (CMU)—i.e., towards system I; these changes result from the action of a fraction of the extract consisting of molecules of small size. The latter changes, which include a marked attenuation of the variable part of fluorescence induction, have been associated with system II and may arise from inhibition of electron flow between water and Q or from decrease in number of functional reaction centers; these changes result from the activity of a proteinaceous fraction of the extract, that simultaneously converts the low temperature steady-state emission spectrum of the chloroplasts into a one-banded one, with maximum at 698 nm.     

Flow cytometry of spinach chloroplasts : determination of intactness and lectin-binding properties of the envelope and the thylakoid membranes

Intact spinach (Spinacia oleracea) chloroplasts, thylakoid membranes, and inside-out or right-side-out thylakoid vesicles have been characterized by flow cytometry with respect to forward angle light scatter, right angle light scatter, and chlorophyll fluorescence. Analysis of intact chloroplasts with respect to forward light scatter and the chlorophyll fluorescence parameter revealed the presence of truly “intact” and “disrupted” chloroplasts. The forward light scatter parameter, normally considered to reflect object size, was instead found to reflect the particle density. One essential advantage of flow cytometry is that additional parameters such as Ricinus communis agglutinin (linked to fluorescein isothiocyanate) fluorescence can be determined through logical conditions placed on bit-maps, amounting to an analytical purification procedure. In the present case, chloroplast subpopulations with fully preserved envelopes, thylakoid membrane, and inside-out or right-side-out thylakoid membranes vesicles can be distinguished. Flow cytometry is also a useful tool to address the question of availability of glycosyl moities on the membrane surfaces if one keeps in mind that organelle-to-organelle interactions could be partially mediated through a recognition process. A high specific binding of R. communis agglutinin and peanut lectin to the chloroplast envelope was detected. This showed that galactose residues were exposed and accessible to specific lectins on the chloroplast surface. No exposed glucose, fucose, or mannose residues could be detected by the appropriate lectins. Ricin binding to the intact chloroplasts caused a strong aggregation. Disruption of these aggregates by resuspension or during passage in the flow cytometer induced partial breakage of the chloroplasts. Only minor binding of R. communis agglutinin and peanut lectin to the purified thylakoid membranes was detected; the binding was found to be low for both inside-out and right-side-out vesicles of the thylakoid membranes.     

The emission yields of delayed and prompt fluorescence from chloroplasts.

1. The decay of delayed fluorescence from chloroplasts blocked with 3-(3,4-dichlorophenyl)-1,1-dimethylurea and uncoupled with gramicidin has been measured in the time range 0.75--45 ms by use of a laser phosphoroscope. 2. The decays have been analysed as the sum of three first-order components of approximate half-lives 0.2, 2.5 and 300 ms by a computer-assisted least-squares fit procedure. 3. The prompt fluorescence yield of the chloroplasts was manipulated by changing the cation concentration of the chloroplast-suspending medium. 4. Analysis of the concentration dependence of the components of the delayed fluorescence decay and of the prompt fluorescence inductions indicates that the emission yield of the intermediate (tau approximately 2.5 ms) component of the decay is equal to the fluorescence yield of a Photosystem II photosynthetic unit with an open trap, and that for the slow (tau approximately 300 ms) component the emission yield is equal to the total Photosystem II prompt fluorescence yield. 5. It is concluded that the delayed fluorescence yield in the time range studied is a complex function of time, which may be due to there being different mechanisms leading to delayed fluorescence production at short and long times after cessation of illumination.     

Fluorescence and Delayed Light Emission from Mesophyll and Bundle Sheath Cells in Leaves of Normal and Salt-Treated Panicum miliaceum

A modified fluorescence microscope system was used to measure chlorophyll fluorescence and delayed light emission from mesophyll and bundle sheath cells in situ in fresh-cut sections from leaves of Panicum miliaceum L. The fluorescence rise in 3-(3,4-dichlorophenyl)-1, 1-dimethylurea (DCMU)-treated leaves and the slow fluorescence kinetics in untreated leaves show that mesophyll chloroplasts have larger photosystem II unit sizes than do bundle sheath chloroplasts. The larger photosystem II units imply more efficient noncyclic electron transport in mesophyll chloroplasts. Quenching of slow fluorescence also differs between the cell types with mesophyll chloroplasts showing complex kinetics and bundle sheath chloroplasts showing a relatively simple decline. Properties of the photosynthetic system were also investigated in leaves from plants grown in soil containing elevated NaCl levels. As judged by changes in both fluorescence kinetics in DCMU-treated leaves and delayed light emission in leaves not exposed to DCMU, salinity altered photosystem II in bundle sheath cells but not in mesophyll cells. This result may indicate different ionic distributions in the two cell types or, alternatively, different responses of the two chloroplast types to environmental change.     

Energization and ultrastructural pattern of thylakoids formed under periodic illumination followed by continuous light

Bean leaves grown under periodic illumination (56 cycles of 2 min light and 98 min darkness) were subsequently exposed to continuous illumination, and in connection with granum formation and accumulation of the light-harvesting pigment-protein complex thermoluminescence and light-induced shrinkage of thylakoid membranes were studied. Juvenile chloroplasts with large double sheets of thylakoids obtained under periodic light exhibited low temperature spectra of polarized fluorescence yielding fluorescence polarization (FP) values < 1 at 695 nm, characteristic for pheophytin emission. In the course of maturation under continuous light when normal grana appeared and the chlorophyll a/b light-harvesting photosystem II complex was incorporated into the membrane, at 695 nm the relative intensity of fluorescence dropped and FP changed to a value of > 1, suggesting an overlap between the emission of pheophytin and that of the chlorophyll a/b light-harvesting photosystem II complex. Thermoluminescence glow curves recorded with juvenile thylakoids displayed a relatively high proportion of emission at low temperatures (around -10°C) while with mature chloroplasts, more thermoluminescence originated from energetically deeper traps (discharged around 28°C). This means that during thylakoid development the capacity of the membrane to stabilize the separated charges increases, which might be favourable for the ultimate conservation of energy. The more extensive energization of mature thylakoids was also indicated by a light-induced decrease in the thickness of the membranes upon illumination; a change which could not be detected in juvenile thylakoids.Abbreviations EDTA ethylenediamine tetraacetic acid - Hepes 4-(2-hydroxy ethyl)-1-piperazine ethane sulfonic acid Dedicated to Prof. L.N.M. Duysens on the occasion of his retirement.     

The relation of millisecond delayed light emission to light-induced ion accumulations in chloroplasts

Delayed fluorescence (delayed light emission) from chloroplasts is increased by ATP, ADP and, to a lesser extent, by ITP. However, neither phosphorylation nor ATP utilization seems to play any part in the phenomenon since the energy transfer inhibitor deoxyphlorizin, which is also an ATPase inhibitor, has no effect on the enhancement of delayed fluorescence. The enhancement of delayed fluorescence by these nucleotides is accompanied by an increase in the extent of proton uptake and n decrease in the nonphosphorylating (basal) electron transport.Uncouplers and ionophores such as imidazole, glycineamide, morpholine, methyl-amine, cyclohexylamine, atebrin, and gramicidin nearly abolish delayed fluorescence. However, ammonium salts are exceptional; they considerably enhance the emission although they also abolish phosphorylation and proton gradient formation. This enhancement of delayed fluorescence occurs only near or above pH 8 and seems to be specific for ammonia when relatively intact lamellae are employed. When particles prepared therefrom with digitonin are used, methylamine also enhances the delayed fluorescence. The enhancement by ammonium salts is correlated with the uptake of ammonium ions. Valinomycin, which is known to increase the permeability of membranes to ammonium ions, abolishes delayed fluorescence in the presence of ammonium salts. It is suggested that (a) ammonia uncoupling abolishes the pH component of the light-induced transmembrane electrochemical potential gradient, but that (b) at higher pH's the electrical component of the gradient (the membrane potential) is not abolished and may even increase while (c) this increased membrane potential is responsible for enhancement of the delayed fluorescence.Gradients which contribute to delayed fluorescence are not necessarily capable of supporting phosphorylation. The requirements for phosphorylation seem more stringent than the requirements for delayed fluorescence and it may be that phosphorylation, unlike the delayed light emission, has an obligatory requirement for a pH gradient.     

Spectral resolution of long term (0.5-50 s) delayed fluorescence from spinach chloroplasts

The emission spectrum of room temperature delayed fluorescence from spinach chloroplasts does not change during the period 0.5-50 s after the cessation of illumination. This provides experimental evidence that charge recombination processes originating in various charge pairs of photosystem II, and manifest as various kinetical components of long term delayed fluorescence, result in the excitation of the same emitters, as predicted by the charge recombination hypothesis.     

Formation kinetics and H2O2 distribution in chloroplasts and protoplasts of photosynthetic leaf cells of higher plants under illumination

The dye H₂DCF-DA, which forms the fluorescent molecule DCF in the reaction with hydrogen peroxide, H₂O₂, was used to study light-induced H₂O₂ production in isolated intact chloroplasts and in protoplasts of mesophyll cells of Arabidopsis, pea, and maize. A technique to follow the kinetics of light-induced H₂O₂ production in the photosynthesizing cells using this dye has been developed. Distribution of DCF fluorescence in these cells in the light has been investigated. It was found that for the first minutes of illumination the intensity of DCF fluorescence increases linearly after a small lag both in isolated chloroplasts and in chloroplasts inside protoplast. In protoplasts of Arabidopsis mutant vtc2-2 with disturbed biosynthesis of ascorbate, the rate of increase in DCF fluorescence intensity in chloroplasts was considerably higher than in protoplasts of the wild type plant. Illumination of protoplasts also led to an increase in DCF fluorescence intensity in mitochondria. Intensity of DCF fluorescence in chloroplasts increased much more rapidly than in cytoplasm. The cessation of cytoplasmic movement under illumination lowered the rate of DCF fluorescence intensity increase in chloroplasts and sharply accelerated it in the cytoplasm. It was revealed that in response to switching off the light, the intensity of fluorescence of both DCF and fluorescent dye FDA increases in the cytoplasm in the vicinity of chloroplasts, while it decreases in the chloroplasts; the opposite changes occur in response to switching on the light again. It was established that these phenomena are connected with proton transport from chloroplasts in the light. In the presence of nigericin, which prevents the establishment of transmembrane proton gradients, the level of DCF fluorescence in cytoplasm was higher and increased more rapidly than in the chloroplasts from the very beginning of illumination. These results imply the presence of H₂O₂ export from chloroplasts to cytoplasm in photosynthesizing cells in the light; the increase in this export falls in the same time interval as does the cessation of cytoplasmic movement.     

Kinetics of chlorophyll fluorescence at 77 K in Chlorella and chloroplasts. Effects of CCCP,ferricyanide and DCMU

The kinetics of chlorophyll fluorescence at 77 K were studied in Chlorella cells and spinach chloroplasts.During a first illumination, the rise is polyphasic with at least three phases. The slowest one is irreversible and corresponds to the cytochrome oxidation.The dark regeneration of half the variable fluorescence is biphasic, the fast phase being inhibited by 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) both in Chlorella and chloroplasts.The fluorescence rise during a second illumination is still biphasic.Carbonyl cyanide m-chlorophenylhydrazone (CCCP) slows down the fluorescence rise in Chlorella but has no effect on the dark regeneration. It does not affect the fluorescence of chloroplasts.Ferricyanide which oxidizes cytochrome b-559 at room temperature produces a quenching of the variable fluorescence and an acceleration of the fluorescence rise during the first illumination.Our results fit the idea of the heterogeneity of the Photosystem II centers at low temperature.     

Long-range interactions of <Emphasis Type="Italic">Chara</Emphasis> chloroplasts are sensitive to plasma-membrane H<Superscript>+</Superscript> flows and comprise separate photo- and dark-operated pathways

Local illumination of the characean internode with a 30-s pulse of white light was found to induce the delayed transient increase of modulated chlorophyll fluorescence in shaded cell parts, provided the analyzed region is located downstream in the cytoplasmic flow at millimeter distances from the light spot. The fluorescence response to photostimulation of a remote cell region indicates that the metabolites produced by source chloroplasts in an illuminated region are carried downstream with the cytoplasmic flow, thus ensuring long-distance communications between anchored plastids in giant internodal cells. The properties of individual stages of metabolite signaling are not yet well known. We show here that the export of assimilates and/or reducing equivalents from the source chloroplasts into the flowing cytoplasm is largely insensitive to the direction of plasma-membrane H⁺ flows, whereas the events in sink regions where these metabolites are delivered to the acceptor chloroplasts under dim light are controlled by H⁺ fluxes across the plasma membrane. The fluorescence response to local illumination of remote cell regions was best pronounced under weak background light and was also observed in a modified form within 1–2 min after the transfer of cell to darkness. The fluorescence transients in darkened cells were suppressed by antimycin A, an inhibitor of electron transfer from ferredoxin to plastoquinone, whereas the fluorescence response under background light was insensitive to this inhibitor. We conclude that the accumulation of reduced metabolites in the stroma leads to the reduction of photosystem II primary quinone acceptor (Q_A) via two separate (photochemical and non-photochemical) pathways.     

The influence of the electric diffusion potential on delayed fluorescence light curves of chloroplasts treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea

The potassium salt-induced transient increase of delayed fluorescence yield was studied in pea chloroplasts treated with 3-(3,4-dichlorophenyl)-1,1-dimethylurea.A simple kinetic model is proposed to account for the actinic light intensity dependence of the delayed fluorescence enhancement by the transmembrane diffusion potential induced by sudden salt addition. The electric field dependence of the rate constants for the recombination of primary separated charges with and without subsequent electronic excitation of reaction center chlorophyll was obtained.From the value of enhancement of delayed fluorescence by salt concentration gradients at saturating actinic light intensity, it is concluded that the distance, normal to thylakoid membrane surface, between the primary acceptor and the donor of Photosystem II is smaller than the membrane thickness.     

Primary Events, Energy Transfer, and Reactions in Photosynthetic Units: Photon Trapping in Photosystem II of Photosynthesis: The Fluorescence Rise Curve in the Presence of 3-(3,4-Dichlorophenyl)-1,1-dimethylurea

Using isolated chloroplasts in the presence of 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), an analysis was made of the rise of the fluorescence yield effected by weak light. Depending on the pretreatment, the time-course of the rapid photochemical part of the rise varied between nearly first-order and quadratic kinetics, i.e., reflected either a one-quantum or a two-quantum conversion. We consider the occurrence of two photoreductants per system II unit, which are reoxidized in different dark reactions. The data further showed that the “first-order process” is also inhomogeneous.