DCMU-INDUCED STIMULATION OF PHOTOSYSTEM I ELECTRON TRANSPORT. INVOLVEMENT OF MEMBRANE STRUCTURAL CHANGES

DCMU-induced stimulation of the rate of photosystem I (PS I) electron transport in DCIPH₂→ MV photoreaction occurs through the action of DCMU on the rate-limiting step which contains the site of electron donation of DCIPH₂ (Ramanujam et al. , 1981). The magnitude of stimulation of the rate by 50 μ M DCMU decreased with increasing concentration of chlorophyll (Chl), implying that DCMU is stoichiometrically related to Chl with respect to the stimulation of the PS I rate.
DCMU-induced stimulation was sensitive to the ionic condition of the thylakoids, the effect being reduced at low cation concentration. Cation-induced scattering changes in thylakoid suspension were partially reversed by DCMU, and the percent Chl in the 10 K fraction of the thylakoid decreased upon addition of DCMU, indicating that grana structure is disrupted by DCMU. Hydroquinone-mediated reduction of cytochrome f in thylakoids in the dark was accelerated in the presence of DCMU. The DCMU effect was not observed in isolated PS I particles.
It is concluded that DCMU binds to the thylakoid membranes and brings about structural changes leading to unstacking of the thylakoids accompanied by an altered interaction of the electron transfer chain components with the added electron donor. This binding of DCMU must have an affinity lower than the well-known binding of DCMU to photosystem II (PS II), because the concentration required is markedly higher.     

ENERGY STORAGE STATES OF PHOTOSYNTHETIC MEMBRANES: ACTIVATION ENERGIES AND LIFETIMES OF ELECTRONS IN THE TRAP STATES BY THERMOLUMINESCENCE METHOD

Abstract Several methods discussed by R. Chen (1969) were used for the calculation of the activation energies ( E ), frequency factors ( s ) and mean lifetimes of electrons in trap states at glow peak temperatures ( T _m) and at room temperature ( T _r) from thermoluminescence glow peaks in spinach chloroplasts and Euglena cells. Results are presented for E calculated independently, i.e. without any assumptions regarding the frequency factors which were determined subsequently using the activation energy values thus calculated. The most reliable values for E , s, r( T _m) and ( T _r) for the well-resolved glow peaks Z(118 K), I(236 K), II(261 K), III(283 K), IV(298 K) and V(321 K) are as follows:
The present comprehensive study has been compared with the earlier ones and the significance of the observed high frequency factors is discussed. It is concluded that only peaks I and II, related to photosystem II, follow the Randall–Wilkins (RW) theory, whereas peaks IV and V, related to photosystem I, do not.     

ON THE ORIGIN OF GLOW PEAKS IN EUGLENA CELLS, SPINACH CHLOROPLASTS AND SUBCHLOROPLAST FRAGMENTS ENRICHED IN SYSTEM I OR II

Abstract— The origin of glow peaks (thermoluminescence) was investigated in isolated spinach chloroplasts and Euglena cells by pretreatment with various concentrations of 3-(3,4 dichlorophenyl)-1,1-dimethylurea (DCMU)?, different light intensities, and after mild heating at various temperatures. Experiments are also reported on subchloroplast fractions enriched in pigment systems I (PSI) or II (PSII) (prepared under conditions to reduce destruction of membranes by excessive detergent contact). These results provide the following, most likely, suggestion for the origin of glow peaks: (1) Z peak originates in metastable states; it is insensitive to DCMU, temperature (320–328 K), and appears only when other peaks are saturated (10 Wm^-2). (2) Peak I involves the use of a reducing entity A (plastoquinone) beyond Q (the primary electron acceptor of pigment system II, PSII), or, of a high “S” state (charge accumulator) of oxygen evolving system; its intensity is dramatically reduced by low concentrations (1 μM) of DCMU, and, there is more of it in PSII than in PSI particles. (3) Peak II is due to reaction of Q^- with the “S” states of the oxygen evolving system; its intensity increases upon the addition of low concentrations of DCMU, at the expense of peak I; it is most sensitive to mild heating, and there is more of it in PSII than in PSI particles. (4) Peak III was not studied here as it was not resolved in most of our preparations. (5) Peak IV is from both pigment system I and II; it is sensitive to heating (>50°C), is somewhat sensitive to DCMU, and is present in both PSI and PSII particles. (6) Peak V is from PSI; it is least sensitive to mild heating, and it is enriched in PSI particles. The present studies have extended our knowledge regarding the origin of glow peaks in spinach chloroplasts and Euglena cells; in particular, the involvement of the charge accumulating “S” states of oxygen evolution (for peaks I and II) and of system I (for peak V) are emphasized in this paper.     

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.     

Effect of doping on thermoluminescence in polymers. I. 9,10-phenanthrenequinone-doped polydiancarbonate

The thermoluminescence (TL) and thermally stimulated depolarization currents (TSDC) observed in polycarbonate doped with 9,10-phenanthrenequinone (PhQ) have been compared in order to test to what extent the TL phenomenon can be correlated with intrinsic relaxation properties of the macromolecular chains. Good qualitative agreement has been found between the two types of curves, showing that the two TL peaks appearing at about 140 and 185 K are attributable to untrapping of electrons induced by the onset of local motions. However, the values and distribution of the activation energies determined by the two techniques differ markedly. The apparent activation energy deduced from TL data presumably reflects the energy level of traps decreased by molecular motions rather than the thermal energy of these relaxations. The primary process responsible for light emission is related to a transition of the n-π type occurring in PhQ at 420 nm, while the trapping sites are probably formed by carbonate groups of the polymeric matrix. The same trapping mechanism has been postulated for the two TL peaks on the basis of their parallel evolutions as a function of dose and dopant concentration.     

PARTICIPATION OF THE TWO PHOTOSYSTEMS IN LIGHT DEPENDENT HYDROGEN EVOLUTION IN Scenedesmus obliquus

Abstract— The H₂-photoproduction in the presence of dithionite measured in wild type and mutant cells of Scenedesmus obliquus demonstrates two sequential phases. In mutants showing only PS I activity phase 1 of H₂-photoproduction is visible with its core activity. When PS II is developed during greening, considerable activity is added to the core of phase I and phase II activity appears. Addition of DCMU reduces H₂-photoproduction by about 90%. The residual activity is completely attributed to the core of phase I. It was concluded that the core of phase I is dependent upon PS I only and can use sources different from water as electron donors. Phase II is dependent upon the capacity of PS II, a functioning photosynthetic apparatus and water as electron donor. The results are supported by studies of wavelength dependent activity of the two separate phases of H₂-photoproduction.     

Assembly of Photosystem I and II during the Early Phases of Light-Induced Development of Chloroplasts from Proplastids in Spirodela oligorrhiza

The aquatic higher plant Spirodela oligorrhiza , which contains proplastids when grown in the dark, was used to study light-dependent chloroplast development. Low-temperature (77 K) and room temperature fluorescence were utilized in situ on whole plants to examine plastid development. The dark-grown plants contain two 77 K fluorescence peaks, at 633 nm (F633) and at 657 nm (F657), with F633 dominating. The F657 species represents protochlorophyllide that is bound to protochloro-phyllide oxidoreductase. It was rapidly phototrans-formed to chlorophyllide (within 5 s) via a monomolec-ular reaction. Free protochlorophyllide (F633) was converted to chlorophyllide during a 3 h exposure to light. Photosystem (PS) assembly in Spirodela could be detected 2 h after the plants were first exposed to light, with the PSII reaction center (77 K fluorescence at 684 nm) appearing slightly before the PSI reaction center (77 K fluorescence at 725 nm). After the first reaction centers were formed the antenna complexes were added; the light-harvesting complex (LHC) I of PSI appeared after 8 h, and 47 kDa chlorophyll protein of PSII appeared between 12 h and 24 h. After 30 h of exposure to light, the plants acquired the ability to perform a light state transition, marking the appearance of functional LHCII complexes in the developing chloroplast. Finally, it was found that photosynthetic activity, as measured by room temperature chlorophyll fluorescence, accelerated con-comitantly with detection of the antenna complexes. Therefore, although reaction centers are detected very early during the proplastid to chloroplast conversion, they may have little activity or be unstable until the antennae are present.     

IN VIVO CHLOROPHYLL a FLUORESCENCE TRANSIENTS AND THE CIRCADIAN RHYTHM OF PHOTOSYNTHESIS IN GONYAULAX POLYEDRA

Abstract— The intensity of chlorophyll a fluorescence during the early part of fluorescence induction at O , initial fluorescence, and P, peak fluorescence, was higher during the day phase of the circadian cycle than during the night phase in continuous light (LL) conditions and was positively correlated with the rate of oxygen evolution. The circadian rhythm in fluorescence in LL persisted in the presence of 10μM 3–(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU), which blocks electron flow from photo-system (PS) II in photosynthesis. The rhythmic changes in fluorescence intensity are consistent with a lower rate constant for radiationless transitions during the day phase than during the night phase of the circadian rhythmicity. The circadian changes in the intensity of fluorescence were abolished at 77K, which may indicate the importance of structural changes in membranes in circadian oscillations.     

Simultaneous Determination of Cadmium,Lead, Copper,and Thallium in Highly Saline Samples by Anodic Stripping Voltammetry (ASV) Using Mercury‐Film and Bismuth‐Film Electrodes

This paper describes a comparative study of the simultaneous determination of Cd(II), Pb(II), Tl(I), and Cu(II) in highly saline samples (seawater, hydrothermal fluids, and dialysis concentrates) by ASV using the mercury‐film electrode (MFE) and the bismuth‐film electrode (BiFE) as working electrodes. The features of MFE and BiFE as working electrodes for the single‐run ASV determinations are shown and their performances are compared with that of HMDE under similar conditions. It was observed that the stripping peak of Tl(I) was well separated from Cd(II) and Pb(II) peaks in all the studied saline samples when MFE was used. Because of the severe overlapping of Bi(III) and Cu(II) stripping peaks in the ASV using BiFE, as well as the overlapping of Pb(II) and Tl(I) stripping peaks in the ASV using HMDE, the simultaneous determination of these metals was not possible in highly saline medium using these both working electrodes. The detection limits calculated for the metals using MFE and BiFE (deposition time of 60 s) were between 0.043 and 0.070 μg L^?1 for Cd(II), between 0.060 and 0.10 μg L^?1 for Pb(II) and between 0.70 and 8.12 μg L^?1 for Tl(I) in the saline samples studied. The detection limits calculated for Cu(II) using the MFE were 0.15 and 0.50 μg L^?1 in seawater/hydrothermal fluid and dialysis concentrate samples, respectively. The methods were applied to the simultaneous determination of Cd(II), Pb(II), Tl(I), and Cu(II) in samples of seawater, hydrothermal fluids and dialysis concentrates.     

DIURNAL VARIATIONS IN LUMINESCENCE IN Scenedesmus obtusiusculus (CHLOROPHYCEAE) INDUCED BY 3-(3,4-DICHLOROPHENYL)-1,1-DIMETHYLUREA

Abstract— Luminescence from synchronously cultured Scenedesmus obtusiusculus cells was measured with a high sensitivity photon counter. Recording of light emission was initiated 0.2 s after switching off actinic light. Luminescence decay was separated into two phases: one for decay to 10⁴ pulses s^-1, the other for decay from 10⁴ to 10³ pulses s^-1. Most photons are emitted during the rapid decay to 10⁴ pulses s^-l. Only small diurnal variations of the two phases could be observed in controls. Treatment with 3-(3,4-dichlorophenyl)-1,1-dimethylurea (DCMU) decreased both the total number of photons emitted and the time required to reach the 10⁴ pulses s^-1 level. No diurnal rhythmicity was induced by DCMU in the first phase but DCMU induced a pronounced diurnal variation in decay time in the second phase of luminescence parallelled by a periodicity in the number of photons emitted. The results indicate that DCMU interferes with the participation of PS I in luminescence. The chlorophyll alb ratio was constant during the life cycle of the cells. No relation could be observed between luminescence and the diurnal rhythmicity in photosynthesis that is characteristic for synchronized unicellular algae.     

THE ROLE OF CYCLIC ELECTRON FLOW AROUND PHOTOSYSTEM I and EXCITATION ENERGY DISTRIBUTION BETWEEN THE PHOTOSYSTEMS UPON ACCLIMATION TO HIGH IONIC STRESS IN Dunaliella salina

Abstract— The distribution of excitation energy between the two photosystems in the halophylic alga Dunaliella salina has been analyzed under ionic stress. In the transition from state 1 to state 2, it was found that a, the absorption cross-section of photosystem (PS) I increased from 42 to 49% until an equal distribution between PS I and PS II was obtained in state 2. Acclimation of the algae to different salt concentrations did not change the fractions of light absorbed in PS II and PS I, but slowed down the transition time from state 1 to state 2. A large increase in ΔpH induced fluorescence quenching was observed which was abolished by the uncoupler nigericin. Photoacoustic quantum yield spectra of energy storage indicated a larger energy storage at 700 nm induced upon stress. The additional ΔpH quenching of fluorescence and the additional quantum yield of energy storage at 700 nm, in the stressed algae, are consistent with the operation of a cyclic, energy-storing pathway in PS I which is uncoupler sensitive.     

APPEARANCE AND DEVELOPMENT OF PHOTOSYNTHETIC ACTIVITIES IN WHEAT ETIOPLASTS GREENED UNDER CONTINUOUS OR INTERMITTENT LIGHT—EVIDENCE FOR WATER-SIDE PHOTOSYSTEM II DEFICIENCY AFTER GREENING UNDER INTERMITTENT LIGHT*

Abstract— Etiolated wheat seedlings are greened under continuous or intermittent light. Under continuous light the onset of photosystem II (PS II) activity appears after 4 h of illumination. Under intermittent light (1 ms flashes alternating with 15 min dark periods), PS II activity cannot be detected after 300–400 flashes, although the pigment composition and structural development of these plastids are similar to those observed after 4 h of continuous light. However, the appearance of PS II activity in isolated plastids can be observed in two different ways: (1) in vivo by exposing the seedlings to a short period of continuous light after the intermittent light; or (2) in vitro by addition to the isolated plastids of an electron donor for PS II, such as diphenylcarbazide. It is concluded that the intermittent light induces development of the electron transport chain from PS II to PS I, but that a deficiency occurs on the water-side of PS II.     

RELATIONSHIP BETWEEN LIGHT-INDUCED STATE I/II-TRANSITIONS and Mg2+-EFFECT ON FLUORESCENCE, TESTED IN SYNCHRONOUS CULTURES OF Scenedesmus obliquus

Abstract— Light induced transition of the photosynthetic apparatus from state II to state I by preillumination with PS I light in vivo and the addition of cations to chloroplasts or chloroplast particles prepared in low-salt buffer have rather similar effects on the fluorescence properties at room temperature and at 77 K. Using synchronous cultures of Scenedesmus obliquus, we were able to study both phenomena in parallel in different developmental stages under well defined conditions. Both phenomena show an inverse course during ontogenetic development of S. obliquus. This result suggests that Mg²⁺ ions and PS I light don't necessarily act in the same way. Hence, changes in the ionic environment cannot be the unique basis of light induced state changes within the photosynthetic apparatus in vivo.     

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.     

光合放氧复合物结构及其放氧机理的研究

光合水氧化是地球上最重要的生化过程之一.光合放氧生物包括光系统Ⅰ(PSⅠ)和光系统Ⅱ(PSⅡ)两种类型反应中心,光系统Ⅱ反应中心能以水作为电子给体,利用光能氧化水产生质子和氧气.对于水如何被氧化这个难题前人已做了大量的工作,但到目前为止放氧复合物(OEC)的结构及水氧化的机理仍不清楚.本文结合当前研究结果,就光合放氧复合物的结构及光合放氧机理进行了综述,希望能有助于推进这方面的工作.     

Wide compositional and structural diversity in the system Tl/Bi/P/Q (Q=S, Se) and observation of vicinal P-Tl J coupling in the solid state

The compounds alpha-TlBiP2Se6 (I), beta-TlBiP2Se6 (II), TlBiP2S6 (III), Tl3Bi3(PS4)4 (IV), TlBiP2S7 (V), and Tl3Bi(PS4)2 (VI) were synthesized, and the structures of I-V were determined by single-crystal X-ray diffraction analysis. The structure of I features infinite chains. Those of compounds II, III, and V are layered. The structure of IV features a three-dimensional framework. Tl4Bi2(PS4)2(P2S6) (VII) was also prepared for comparison to the title compounds. The band gaps of each compound are 1.23, 1.27, 1.81, 1.88, 2.06, 1.98, and 1.97 eV for I-VII, respectively. Compounds I, III, IV, and VI melt congruently at 544, 595, 495, and 563 degrees C, respectively, and compounds II, V, and VII melt incongruently at 544, 509, and 600 degrees C, respectively. Solid-state 31P NMR spectroscopy of the reported compounds demonstrates chemical shifts and chemical shift anisotropies in line with related chalcophosphate materials. Evidence for two-bond P-Tl J coupling was observed in 31P NMR spectra (J=481-1781 Hz), and to the best of our knowledge, this is the first example of two-bond P-Tl J coupling and the first example of P-Tl coupling in the solid state. It was possible to assign chemical shifts of inequivalent 31P atoms from the same [PxQy]z- anion type based on different modes of metal ion coordination to the chalcogen. These assignments provide information about the vicinal metal ion contribution to the 31P chemical shift.     

THE COMPLEXITY OF THE FLUORESCENCE OF CHLORELLA PYRENOIDOSA

Abstract— The complexity of the room-temperature emission spectrum of Chlorella was investigated by a matrix analysis method. This approach revealed the presence of two independently fluorescent components in the short-wave region of the spectrum. These components, maximal at about 687 and 695 nm, appeared to correspond to the fluorescence of the bulk pigments of PS II and PS I respectively. The analysis was insensitive to the individual species within the photosystems. As such, other minor fluorescent species, usually observed at low temperatures, which presumably correspond to fluorescence from the trapping centres, did not appreciably complicate the analysis. The absorption spectra of the two photosystems were calculated from the fluorescence data. The results were similar to those that have been obtained by other workers from oxygen evolution and DCMU poisoning data but differed from those obtained by computer analysis of the absorption spectrum. Addition of reduced DCPIP was observed to reverse the increase in fluorescence yield and changes in the spectral distribution of emission taking place on poisoning the algae. The correlation between this and the catalysis of photophos-phorylation in aged or poisoned chloroplasts was noted. This correlation was tentatively interpreted as evidence for a direct interaction between the donor system and the photochemical apparatus associated with PS II, rather than with a member of the electron transport chain as is normally assumed.     

Annual variation in photo acclimation and photoprotection of the photobiont in the foliose lichen Xanthoria parietina

Seasonal variation in maximal photochemical quantum yield (F(V)/F(M)) of photosystem II (PS II), light adapted quantum yield (Phi(II)) of PS II, non-photochemical quenching (NPQ), contents of chlorophylls, and xanthophyll cycle pigments (VAZ) was studied in Xanthoria parietina repeatedly sampled in one location in S Norway during one year. The seasonal course in the susceptibility to photoinhibition was evaluated as high light-induced changes (1,800 micromol photons m(-2) s(-1) for 24h) in F(V)/F(M), Phi(II), and NPQ, measured as the ability to recover after 2 and 20 h at low light in control thalli with a natural cortical parietin screen, and in thalli from which parietin had been removed prior to high light exposures. F(V)/F(M), Phi(II), chlorophyll content, and the conversion state of VAZ (DEPS) reached minimum in spring. At the same time, yearly maxima of VAZ content and NPQ were recorded. Thereafter, F(V)/F(M), Phi(II), and chlorophyll content increased gradually, reaching maximum values in late autumn. DEPS peaked already in summer. Similarly, VAZ and NPQ decreased from early summer until winter. All data show that the X. parietina photobiont acclimates to seasonal changes in solar radiation, consistent with the lichen's preference for well-lit habitats. However, a comparison with a study of seasonal acclimation in the X. parietina mycobiont shows that in order to understand the seasonal photobiont acclimation, one has to consider the seasonal variation in internal screening caused by the fungal regulation of the PAR-absorbing parietin. A joint effort of both bionts seems to be required to avoid serious photoinhibition.     

Changes in the energy distribution between chlorophyll-protein complexes of thylakoid membranes from pea mutants with modified pigment content. I. Changes due to the modified pigment content

The low-temperature (77 K) emission and excitation chlorophyll fluorescence spectra in thylakoid membranes isolated from pea mutants were investigated. The mutants have modified pigment content, structural organization, different surface electric properties and functions [Dobrikova et al., Photosynth. Res. 65 (2000) 165]. The emission spectra of thylakoid membranes were decomposed into bands belonging to the main pigment protein complexes. By an integration of the areas under them, the changes in the energy distribution between the two photosystems as well as within each one of them were estimated. It was shown that the excitation energy flow to the light harvesting, core antenna and RC complexes of photosystem II increases with the total amount of pigments in the mutants, relative to the that to photosystem I complexes. A reduction of the fluorescence ratio between aggregated trimers of LHC II and its trimeric and monomeric forms with the increase of the pigment content (chlorophyll a, chlorophyll b, and lutein) was observed. This implies that the closer packing in the complexes with a higher extent of aggregation regulates the energy distribution to the PS II core antenna and reaction centers complexes. Based on the reduced energy flow to PS II, i.e., the relative increased energy flow to PS I, we hypothesize that aggregation of LHC II switches the energy flow toward LHC I. These results suggest an additive regulatory mechanism, which redistributes the excitation energy between the two photosystems and operates at non-excess light intensities but at reduced pigment content.     

Electron transfer reactions of redox cofactors in spinach photosystem I reaction center protein in lipid films on electrodes

Thin film voltammetry was used to obtain direct, reversible, electron transfer between electrodes and spinach Photosystem I reaction center (PS I) in lipid films for the first time. This reaction center (RC) protein retains its native conformation in the films, and AFM showed that film structure rearranges during the first several minutes of rehydration of the film. Two well-defined chemically reversible reduction-oxidation peaks were observed for native PS I in the dimyristoylphosphatidylcholine films, and were assigned to phylloquinone, A(1) (E(m) = -0.54 V) and iron-sulfur clusters, F(A)/F(B) (E(m) = -0.19 V) by comparisons with PS I samples selectively depleted of these cofactors. Observed E(m) values may be influenced by protein-lipid interactions and electrode double-layer effects. Voltammetry was consistent with simple kinetically limited electron transfers, and analysis of reduction-oxidation peak separations gave electrochemical rate constants of 7.2 s(-)(1) for A(1) and 65 s(-)(1) for F(A)/F(B). A catalytic process was observed in which electrons were injected from PS I in films to ferredoxin in solution, mimicking in vivo electron shuttle from the terminal F(A)/F(B) cofactors to soluble ferredoxin during photosynthesis.