Correlation between lifetime heterogeneity and kinetics heterogeneity during chlorophyll fluorescence induction in leaves: 2. Multi-frequency phase and modulation analysis evidences a loosely connected PSII pigment-protein complex

We report the first direct decomposition of the fluorescence lifetime heterogeneity during multiphasic fluorescence induction in dark-adapted leaves by multi-frequency phase and modulation fluorometry (PMF). A very fast component, assigned to photosystem I (PSI), was found to be constant in lifetime and yield, whereas the two slow components, which are strongly affected by the closure of the reaction centers by light, were assigned to PSII. Based on a modified “reversible radical pair” kinetic model with three compartments, we showed that a loosely connected pigment complex, which is assumed to be the CP47 complex, plays a specific role with respect to the structure and function of the PSII: (i) it explains the heterogeneity of PSII fluorescence lifetime as a compartmentation of excitation energy in the antenna, (ii) it is the site of a conformational change in the first second of illumination, and (iii) it is involved in the mechanisms of nonphotochemical quenching (NPQ). On the basis of the multi-frequency PMF analysis, we reconciled two apparently antagonistic aspects of chlorophyll a fluorescence in vivo: it is heterogeneous with respect to the kinetic structure (several lifetime components) and homogeneous with respect to average quantities (quasi-linear mean τ-Φ relationship).     

Effect of photosystem II reaction center closure on nanosecond fluorescence relaxation kinetics

The fluorescence decay of chlorophyll in spinach thylakoids was measured as a function of the degree of closure of Photosystem II reaction centers, which was set for the flowed sample by varying either the preillumination by actinic light or the exposure of the sample to the exciting pulsed laser light. Three exponential kinetic components originating in Photosystem II were fitted to the decays; a fourth component arising from Photosystem I was determined to be negligible at the emission wavelength of 685 nm at which the fluorescence decays were measured. Both the lifetimes and the amplitudes of the components vary with reaction center closure. A fast (170–330 ps) component reflects the trapping kinetics of open Photosystem II reaction centers capable of reducing the plastoquinone pool; its amplitude decreases gradually with trap closure, which is incompatible with the concept of photosynthetic unit connectivity where excitation energy which encounters a closed trap can find a different, possibly open one. For a connected system, the amplitude of the fast fluorescence component is expected to remain constant. The slow component (1.7–3.0 ns) is virtually absent when the reaction centers are open, and its growth is attributable to the appearance of closed centers. The middle component (0.4–1.7 ns) with approximately constant amplitude may originate from centers that are not functionally linked to the plastoquinone pool. To explain the continuous increase in the lifetimes of all three components upon reaction center closure, we propose that the transmembrane electric field generated by photosynthetic turnover modulates the trapping kinetics in Photosystem II and thereby affects the excited state lifetime in the antenna in the trap-limited case.Abbreviations DCMU 3-(3,4-dichlorophenyl)-1,1-dimethylurea - HEPES 4-(2-hydroxyethyl)-1-piperazineethane sulfonic acid - PQ plastoquinone - PSI and PSII Photosystem I and II - Q_A and Q_B primary and secondary quinone acceptor of PSII     

Probing Photosynthesis on a Picosecond Time Scale: Evidence for Photosystem I and Photosystem II Fluorescence in Chloroplasts

Fluorescent emission kinetics of isolated spinach chloroplasts have been observed at room temperature with an instrument resolution time of 10 ps using a frequency doubled, mode-locked Nd:glass laser and an optical Kerr gate. At 685 nm two maxima are apparent in the time dependency of the fluorescence; the first occurs at 15 ps and the second at 90 ps after the flash. The intervening minimum occurs at about 50 ps. On the basis of theoretical models, lifetimes of the components associated with the two peaks and spectra (in escarole chloroplasts), the fluorescence associated with the first peak is interpreted as originating from Photosystem I (PSI) (risetime ≤10 ps, lifetime ≤10 ps) and the second peak from Photosystem II (PSII) (lifetime, 210 ps in spinach chloroplasts and 320 ps in escarole chloroplasts). The fact that there are two fluorescing components with a quantum yield ratio ≤0.048 explains the previous discrepancy between the quantum yield of fluorescence measured in chloroplasts directly and that calculated from the lifetime of PSII. The 90 ps delay in the peak of PSII fluorescence is probably explained by energy transfer between accessory pigments such as carotenoids and Chl a. Energy spillover between PSI and PSII is not apparent during the time of observation. The results of this work support the view that the transfer of excitation energy to the trap complex in both photosystems occurs by means of a molecular excitation mechanism of intermediate coupling strength. Although triplet states are not of major importance in energy transfer to PSII traps, the possibility that they are involved in PSI photochemistry has not been eliminated.     

Functional and Structural Organization of Chlorophyll in the Developing Photosynthetic Membranes of Euglena gracilis Z: II. CHARACTERISTICS OF THE LATE FORMATION OF ACTIVE PHOTOSYSTEM II REACTION CENTERS DURING FIRST STAGES OF GREENING

During light-induced greening of dark-grown, nondividing Euglena gracilis Z, there is a delay of about 10 hours in the formation of active photosystem II (PSII) reaction centers compared to chlorophyll synthesis. Experiments with greening under different light intensities rule out the possibility that this delay results from a late induction of active PSII reaction center formation when a definite amount of chlorophyll is attained in the early greened cells. Experiments on greening after preillumination show that this delay does not originate in a long, light-induced formation of specific synthesizing machinery for reaction center components. Experiments with greening in the presence of streptomycin show that, when this inhibitor of protein synthesis by chloroplastic ribosomes is added to dark-grown, preilluminated cells or to cells already greened for 24 hours, the formation of active PSII reaction centers is inhibited after a time which depends on the light intensity used for greening. Under very low light intensity (150 lux), the addition of streptomycin to 24-hour greened cells does not prevent further development of functional chloroplasts. These observations lead to the conclusion that streptomycin-insensitive chloro-plast development occurs due to syntheses of cytoplasmic origin and of light-induced pools of components synthesized early by chloroplastic ribo-somes. Conformational changes requiring time may allow the insertion of components necessary for the reorganization of PSII reaction centers in the developing thylakoid after synthesis. This hypothesis accounts for the observed delay in PSII reaction center formation compared to chlorophyll synthesis.     

Evidence that the variable chlorophyll fluorescence in Chlamydomonas reinhardtii is not recombination luminescence

Room temperature single photon timing measurements on intact, Chlamydomonas reinhardtii cells at low excitation energies have been analysed using a four exponential kinetic model. Closing the PSII reaction centres produced two major variable lifetime and two minor constant lifetime components. The yield of each component mirrored the changes in lifetime. Such observations indicate the presence of well-connected PSII centres favoring excitation energy transfer. A Chlamydomonas mutant lacking PSII reaction centre proteins exhibited decay components equivalent to those seen at F_M in the wild-type. A titration of in vivo fluorescence, in both the mutant and wild-type algae, using DNB, produced decay components similar to those seen on opening PSII reaction centres. Such observations indicate that the luminescence hypothesis for the origin of the long-lived lifetime component is not the case.Abbreviations DCMU 3-(3,4-dichlorophenyl)-1, 1-dimethyl urea - DNB m,Dinitrobenzene - PSII photosystem II - RCII PSII recation centre - I^- reduced pheophytin - Q_A primary stable electron ecceptor of PSII - Ch1 chlorophyl1 - LHCII light harvesting Ch1a/b protein complex of PSII - F_O initial fluorescence level - F_M maximum fluorescence level - F_V variable fluorescence (F_M-F_O) - ps picosecond - ns nanosecond     

A retrieval algorithm to evaluate the Photosystem I and Photosystem II spectral contributions to leaf chlorophyll fluorescence at physiological temperatures

A new computational procedure to resolve the contribution of Photosystem I (PSI) and Photosystem II (PSII) to the leaf chlorophyll fluorescence emission spectra at room temperature has been developed. It is based on the Principal Component Analysis (PCA) of the leaf fluorescence emission spectra measured during the OI photochemical phase of fluorescence induction kinetics. During this phase, we can assume that only two spectral components are present, one of which is constant (PSI) and the other variable in intensity (PSII). Application of the PCA method to the measured fluorescence emission spectra of Ficus benjamina L. evidences that the temporal variation in the spectra can be ascribed to a single spectral component (the first principal component extracted by PCA), which can be considered to be a good approximation of the PSII fluorescence emission spectrum. The PSI fluorescence emission spectrum was deduced by difference between measured spectra and the first principal component. A single-band spectrum for the PSI fluorescence emission, peaked at about 735?nm, and a 2-band spectrum with maxima at 685 and 740?nm for the PSII were obtained. A linear combination of only these two spectral shapes produced a good fit for any measured emission spectrum of the leaf under investigation and can be used to obtain the fluorescence emission contributions of photosystems under different conditions. With the use of our approach, the dynamics of energy distribution between the two photosystems, such as state transition, can be monitored in vivo, directly at physiological temperatures. Separation of the PSI and PSII emission components can improve the understanding of the fluorescence signal changes induced by environmental factors or stress conditions on plants.     

Chlorophyll organization in dark-grown and light-grown pine (Pinus brutia) and barley (Hordeum vulgare)

A study was conducted comparing the organization of chlorophyll during development of the photosynthetic apparatus in dark-grown and light-grown pine and barley. The rationale was that gymnosperms, but not angiosperms, have a capacity to synthesize chlorophyll in darkness. Seedlings of Pinus brutia were germinated and grown in darkness or under photoperiodic (day/night) conditions. The low-temperature (77 K) fluorescence spectra of newly-emerging dark-grown seedlings exhibited a single fluorescence band peaking at 678–679 nm, which decayed primarily with a ∼5.5 ns lifetime. Over the first few days of growth, the emission shifted to longer wavelengths and a subnanosecond lifetime component became prevalent. After several days of dark growth the emission spectrum and lifetime profile of the low temperature fluorescence came to resemble those of light-grown pine and barley. At room temperature, dark-grown pine showed little variable fluorescence, though addition of DCMU caused a substantial fluorescence rise. Illumination with moderate light for a few hours was sufficient to 'photoinduce' the appearance of normal variable fluorescence. At 77 K, DCMU-treated samples clearly showed a very long-lived (∼40 ns) fluorescence lifetime component in light-grown pine and barley. This component was undetectable in dark-grown pine. If, however, dark-grown samples were illuminated either before or after DCMU addition and then frozen to 77 K, the ∼40 ns lifetime component appeared at a fluorescence intensity similar to that in light-grown samples. These results are explained primarily in terms of photoactivation of the photosystem II (PSII) donor side. The temporary maintenance of PSII in an inactive, highly-quenched state is suggested to provide an available, yet protected precursor for active PSII.     

Picosecond Time-Resolved Fluorescence from Detergent-Free Photosystem I Particles

Picosecond time-resolved fluorescence measurements have been taken on a detergent-free P700-enriched complex at room temperature isolated from the blue-green alga Phormidium luridum with a chlorophyll a to reaction center ratio of 100. Emission at greater than 665 nm is characterized by two exponential-decay components. A fast component, which dominates the initial decay with an average lifetime of 16 ps and 87% amplitude, is attributed to excitations in the core antenna chlorophyll-proteins, which are rapidly trapped by the primary electron donor, P700. A second component, with an average lifetime of 106 ps and 13% amplitude, is attributed to the peripheral antenna proteins. For 532-nm, 30-ps pulse excitation the results are virtually independent of fluence in the range of 2 × 10¹² to 4 × 10¹⁶ photons/cm² and the oxidation state of P700. Addition of sodium dodecyl sulfate to 0.1% causes the second component's lifetime to increase by an average of a factor of 2.5. Only minor changes are observed in the first component's lifetime and the relative amplitudes of the two components. Two fractions isolated from the detergent-treated samples have also been examined. Our results indicate that excitation energy transfer within photosystem I is very efficient and that the excitation kinetics of the antennae may be limited by the trapping rate of P700 or strongly affected by the heterogeneity of the antennae.     

Identification of assembly precursors to photosystems emitting fluorescence at 683 nm and 687 nm by cryogenic fluorescence microspectroscopy

Photosystem I (PSI) and photosystem II (PSII) play key roles in photoinduced electron-transfer reaction in oxygenic photosynthesis. Assemblies of these PSs can be initiated by illumination of the etiolated seedlings (greening). The study aimed to identify specific fluorescence spectral components relevant to PSI and PSII assembly intermediates emerging in greening seedlings of Zea mays, a typical C4 plant. The different PSII contents between the bundle sheath (BS) and mesophyll (M) cells were utilized to spectrally isolate the precursors to PSI and PSII. The greening Zea mays leaf thin sections were observed with the cryogenic microscope combined with a spectrometer. With the aid of the singular-value decomposition analysis, we could identify four independent fluorescent species, SAS677, SAS685, SAS683, and SAS687, named after their fluorescence peak wavelengths. SAS677 and SAS685 are the dominant components after the 30-minute greening, and the distributions of these components showed no clear differences between M and BS cells, indicating immature cell differentiation in this developing stage. On the other hand, the 1-hour greening resulted in reduced distributions of SAS683 in BS cells leading us to assign this species to PSII precursors. The 2-hour greening induced the enrichment of SAS687 in BS cells suggesting its PSI relevance. Similarity in the peak wavelengths of SAS683 and the reported reaction center of PSII implied their connection. SAS687 showed an intense sub-band at around 740 nm, which can be assigned to the emission from the red chlorophylls specific to the mature PSI.     

Effect of Elevated Temperatures on the Activity of Alternative Pathways of Photosynthetic Electron Transport in Intact Barley and Maize Leaves

The light-induced rise in chlorophyll fluorescence and the subsequent decay of fluorescence in darkness were measured in barley and maize leaves exposed to heat treatment. The redox conversions of the photosystem I primary donor P700, induced by far-red light, were also monitored from the absorbance changes at 830 nm. After heating of leaves at temperatures above 40°C, the ratio of variable and maximum fluorescence decreased for leaves of both plant species, indicating the inhibition of photosystem II (PSII) activity. A twofold reduction of this ratio in barley and maize leaves was observed after heating at 45.3 and 48.1°C, respectively, which suggests the higher functional resistance of PSII in maize. The amplitude of the slow phase in the dark relaxation of variable fluorescence did not change after the treatment of barley and maize leaves at temperatures up to 48°C. In leaves treated at 42 and 46°C, the slow phase of dark relaxation deviated from an exponential curve. The relaxation kinetics included a temporary increase in fluorescence to a peak about 1 s after turning off the actinic light. Unlike the slow component, the fast and intermediate phases in the dark relaxation of variable fluorescence disappeared fully or partly after the treatment of leaves at 46°C. The photooxidation of P700 in heat-treated leaves was saturated at much higher irradiances of far-red light than in untreated leaves. At the same time, the dark reduction of P700⁺ was substantially accelerated after heat treatment. The data provide evidence that the heating of leaves stimulated the alternative pathways of electron transport, i.e., cyclic transport around photosystem I and/or the donation of electrons to the plastoquinone pool from the reduced compounds located in the chloroplast stroma. The rate of alternative electron transport after the heat treatment was higher in maize leaves than in barley leaves. It is supposed that the stimulation of alternative electron transport, associated with proton pumping into the thylakoid, represents a protective mechanism that prevents the photoinhibition of PSII in leaves upon a strong suppression of linear electron transport in chloroplasts exposed to heat treatment.     

Functional and Structural Organization of Chlorophyll in the Developing Photosynthetic Membranes of Euglena gracilis Z: III. SEQUENCE OF EVENTS LEADING TO THE FORMATION OF FUNCTIONAL PHOTOSYSTEM II PHOTOSYNTHETIC UNITS

Greening cells of Euglena were transferred back to darkness at different stages of chloroplast development in the presence or absence of specific inhibitors of protein synthesis. The analysis of chloroplast components showed that: (a) cycloheximide or streptomycin does not significantly inhibit the formation in darkness of active photosystem II (PSII) reaction centers if added after the lag phase for chloroplast development; (b) a limited number of active reaction centers are formed in the dark, sufficient to increase PSII reaction center to chlorophyll ratios to values close to those found in fully greened cells; (c) these dark-formed reaction centers appear to be inserted in already constituted and complete light-harvesting antennae. These results complement previous ones and lead us to propose a model for a sequential formation of PSII photosynthetic units during greening of Euglena, whereby conformational changes requiring time would allow already synthesized components of PSII reaction centers to be inserted or reorganized as active photochemical complexes in association with previously formed light-harvesting antennae.     

Fluorescence Properties Indicate that Photosystem II Reaction Centers and Light-Harvesting Complex Are Modified by Low Temperature Growth in Winter Rye

Thylakoids isolated from winter rye (Secale cereale L. cv Puma) grown at 20°C (nonhardened rye, RNH) or 5°C (cold-hardened rye, RH) were characterized using chlorophyll (Chl) fluorescence. Low temperature fluorescence emission spectra of RH thylakoids contained emission bands at 680 and 695 nanometers not present in RNH thylakoids which were interpreted as changes in the association of light-harvesting Chl a/b proteins and photosystem II (PSII) reaction centers. RH thylakoids also exhibited a decrease in the emission ratio of 742/685 nanometers relative to RNH thylakoids.

Room temperature fluorescence induction revealed that a larger proportion of Chl in RH thylakoids was inactive in transferring energy to PSII reaction centers when compared with RNH thylakoids. Fluorescence induction kinetics at 20°C indicated that RNH and RH thylakoids contained the same proportions of fast (α) and slow (β) components of the biphasic induction curve. In RH thylakoids, however, the rate constant for α components increased and the rate constant for β components decreased relative to RNH thylakoids. Thus, energy was transferred more quickly within a PSII reaction center complex in RH thylakoids. In addition, PSII reaction centers in RH thylakoids were less connected, thus reducing energy transfers between reaction center complexes. We concluded that both PSII reaction centers and light-harvesting Chl a/b proteins had been modified during development of rye chloroplasts at 5°C.

     

Fluorescence induction of Photosystem II membranes shows the steps till reduction and protonation of the quinone pool

Chlorophyll fluorescence induction (Chl-F) was investigated in Photosystem II (PSII)-enriched membranes, which predominantly include active (Q_B reducing) PSII reaction centres (RCs) and lack Photosystem I (PSI). The Chl-F curve of these preparations show a polyphasic rise from F₀, the minimal fluorescence, to F_P, the maximal fluorescence, with several intermediate transitions. Analyses of these transitions revealed three exponential rise components with lifetimes of 18 ms, 400 ms and 800 ms. The 18 ms component was assigned to the photoaccumulation of reduced Q_A. The two slowest components, of 400 ms and 800 ms, were assigned to Q_B reduction (Q_B⁻ and Q_B⁼) and further Q_B⁼ protonation (till Q_BH₂), respectively. These assignments were based on the observation of specific quenching of the phases by DCMU or by different oxidized, reduced and protonated quinones. The work is done in low light conditions which are saturating to avoid photoinhibition or PSII inactivation effects. The results suggest that the Chl-F curve observed in PSII-enriched membranes can be attributed to the sequential steps till the photoaccumulation (reduction and protonation) of plastoquinone (PQ) by PSII. These results are in good agreement with the molecular models that show a correspondence between Chl-F and PQ reduction steps, like the models that propose and explain the O-J-I-P transients.     

Biogenesis of Thylakoid Membranes in Chlamydomonas reinhardtii y1 (A Kinetic Study of Initial Greening)

Initiation of thylakoid membrane assembly was examined in degreened cells of Chlamydomonas reinhardtii y1 cells depleted of thylakoid membranes and photosynthetic activity by growth in the dark for 3 to 4 d. Photoreductive activities of photosystem II (PSII) and photosystem I (PSI) increased with no apparent lag when degreened cells were exposed to light at 38[deg]C. However, fluorescence transients induced by actinic light, which reflect the functional state of PSII, changed only slightly during the first 2 h of greening. When these cells were treated with 3-(3,4-dichlorophenyl)-1,1-dimethyl urea (DCMU) or saturating light, fluorescence increased commensurate with the cellular content of chlorophyll. In similar experiments with greening cells of C. reinhardtii CC-2341 (ac-u-g-2.3), a PSI-minus strain, fluorescence increased with chlorophyll without treatment with DCMU. These data suggested that fluorescence of initial PSII centers in greening y1 cells was quenched by activity of PSI. Continuous monitoring of fluorescence in the presence or absence of DCMU showed that assembly of quenched PSII centers occurred within seconds after exposure of y1 cells to light. These results are consistent with initial assembly of PSI and PSII within localized domains, where their proximity allows efficient energy coupling.     

Resolution of Fluorescence Emission Spectra with Various Lifetime Components of D1/D2/Cyt b-559

PS Ⅱ reaction center D1/D2/Cyt b-559 purified from chloroplasts of spinach has four components of fluorescence decaying with lifetimes of 1.0 ns, 5.9 ns,24 ns,and 73 ns whose fractions to total fluorescence yield are 0. 05,0.34,0. 35 and 0.26 respectively. The fluorescence emission spectra of these lifetime components are closely overlapping, and only one peak is shown in steady state emission spectrum. Based on the hardware analysis of phase fluorometry,by selection of the detector phase angle,the emission from various components could be individually suppressed. If the 5.9 ns component was suppressed, the emission spectrum was red-shifted. On the contrary, the emission spectrum was blue-shifted when 73 ns component was suppressed. Based on the software analysis, the individual emission spectra were resolved with three lifetime components by measuring phase and modulation data at various wavelength. Compared with steady state spectrum,the emission maximum wavelength of 5.9 ns component was blue-shifted from 68nm to 680 nm,but those of 24 ns and 73 ns components were red-shifted to 685 nm and 683 nm respectively.     

Diagnosis of the Earliest Strain-Specific Interactions between Tobacco Mosaic Virus and Chloroplasts of Tobacco Leaves in Vivo by Means of Chlorophyll Fluorescence Imaging

Fluorescence imaging was used to diagnose early stages of the strain-specific interactions between tobacco mosaic virus (strain PV230) and chloroplasts following infection of tobacco leaves (Nicotiana tabacum cv Xanthi). The earliest indication of interaction in tissues that ultimately become chlorotic was a reduction in chlorophyll fluorescence, and there was little fluorescence quenching compared with adjacent healthy tissues. Subsequently, fluorescence increased but remained unquenched. In the late stages fluorescence declined again in chlorotic regions as the chloroticmosaic symptoms developed. These in vivo data showing altered fluorescence yields confirm strain-specific interaction of virus coat protein with photosystem II (PSII) components in vitro, leading to photoinhibition and photooxidation of chlorophyll in infected cells and the development of visible chlorotic-mosaic symptoms. Although mechanisms leading to the low, unquenched fluorescence condition are not known, the intermediate high, unquenched fluorescence condition is consistent with impaired PSII electron transport as measured in vitro. Fluorescence lesions appear more rapidly and develop more extensively in high light, consistent with the faster and larger extent of symptom formation in high-light-grown leaves than in low-light-grown leaves.     

Probing the Dynamics of Doxorubicin-DNA Intercalation during the Initial Activation of Apoptosis by Fluorescence Lifetime Imaging Microscopy (FLIM)

Doxorubicin is a potent anthracycline antibiotic, commonly used to treat a wide range of cancers. Although postulated to intercalate between DNA bases, many of the details of doxorubicin’s mechanism of action remain unclear. In this work, we demonstrate the ability of fluorescence lifetime imaging microscopy (FLIM) to dynamically monitor doxorubicin-DNA intercalation during the earliest stages of apoptosis. The fluorescence lifetime of doxorubicin in nuclei is found to decrease rapidly during the first 2 hours following drug administration, suggesting significant changes in the doxorubicin-DNA binding site’s microenvironment upon apoptosis initiation. Decreases in doxorubicin fluorescence lifetimes were found to be concurrent with increases in phosphorylation of H2AX (an immediate signal of DNA double-strand breakage), but preceded activation of caspase-3 (a late signature of apoptosis) by more than 150 minutes. Time-dependent doxorubicin FLIM analyses of the effects of pretreating cells with either Cyclopentylidene-[4-(4-chlorophenyl)thiazol-2-yl)-hydrazine (a histone acetyltransferase inhibitor) or Trichostatin A (a histone deacetylase inhibitor) revealed significant correlation of fluorescence lifetime with the stage of chromatin decondensation. Taken together, our findings suggest that monitoring the dynamics of doxorubicin fluorescence lifetimes can provide valuable information during the earliest phases of doxorubicin-induced apoptosis; and implicate that FLIM can serve as a sensitive, high-resolution tool for the elucidation of intercellular mechanisms and kinetics of anti-cancer drugs that bear fluorescent moieties.     

Oxygenic photoreduction of methyl viologen and nicotinamide adenine dinucleotide phosphate without the involvement of photosystem I during plastid development

Studies on the appearance of various electron transport functions were followed during greening of etiolated cucumber cotyledons. Appearance of dichlorodimethoxy-p-benzoquinone, dimethyl quinone, tetramethyl-p-phenylenediamine, dichlorophenol indophenol and ferricyanide Hill reactions were observed after 8h of greening. However, photoreduction of methyl viologen (MV) and nicotinamide adenine dinucleotide phosphate (NADP) was observed from 2h of greening. Variable fluorescence, which is a direct indication of water-splitting function, was observed from 2h of greening in cotyledons, thylakoid membranes and photosystem II (PSII) particles. The decrease in variable fluorescence in the presence of MV (due to rapid reoxidation of Q-) observed from early stages of greening confirmed the photoreduction of MV by PSII. The early development of water-splitting function was further confirmed by the abolition of variable fluorescence in thylakoid membranes and PSII particles by heat treatment and concomittant loss of light dependent oxygen uptake in the presence of MV in heat treated chloroplasts. However, the photoreduction of MV and NADP was insensitive to intersystem electron transport inhibitors, dichlorophenyl dimethylurea or dibromomethyl isopropyl-p-benzoquinone till 8h of greening. Though the oxidation of intersystem electron carrier cytochrome f was observed from early stages of greening, the reduction of cytochrome f was not observed till 8h of greening. All these observations confirm that during early stages of greening MV and NADP are photoreduced by PSII without the involvement of intersystem electron carriers or the collaboration of PSI. Since these observations are at variance with the currently prevalent concept (Z-Scheme) of the photosynthetic generation of reducing power, which requires definite collaboration of the two photosystems, an alternate electron flow pathway is proposed.     

Kinetic evidence for two Na channels in frog skeletal muscle

The kinetics of voltage-clamped sodium currents were studied in frog skeletal muscle. Sodium currents in frog skeletal muscle activate and inactivate following an initial delay in response to a depolarizing voltage pulse. Inactivation occurs via a double exponential decay exhibiting fast and slow components for virtually all depolarizing pulses used.The deactivation of Na currents exhibits two exponential components, one decaying rapidly, while the other decays slowly in time; the relative amplitude of the two components changes with the duration of the activating pulse. The two deactivation phases remain after pharmacological elimination of inactivation.In individual fibers, the percent amplitude of the slow inactivation component correlates with the percent amplitude of the slow deactivation component.Tetrodotoxin differentially blocks the slow deactivation component.These observations are interpreted as the activation, inactivation and deactivation of two subtypes (fast and slow) of Na channels.Studies of the slow deactivation phase magnitude vs the duration of the eliciting pulse provide a way to determine the kinetics of the slow Na channel in muscle.Ammonium substitution for Na in the Ringer produces a voltage dependent activation and inactivation of current which exhibits only one decay phase, and eliminates the slow decay phase of current, suggesting that adjustments of the ionic environment of the channels can mask the presence of one of the channel subtypes.     

Studies on Chromophore Coupling in Isolated Phycobiliproteins: II. Picosecond Energy Transfer Kinetics and Time-Resolved Fluorescence Spectra of C-Phycocyanin from Synechococcus 6301 as a Function of the Aggregation State

The fluorescence kinetics of C-Phycocyanin in the monomeric, trimeric, and hexameric aggregation states has been measured as a function of the emission wavelength with picosecond resolution using the single-photon timing technique. All the decay curves measured at the various emission wavelengths were analyzed simultaneously by a global data analysis procedure. A sum of four exponentials was required to fit the data for the monomers and trimers. Only in the case of the hexamers, a three-exponential model function proved to be nearly sufficient to describe the experimental decays. The lifetime of those fluorescence components reflecting energy transfer decreased with increasing aggregation. This is due to the increased number of efficient acceptor molecules next to a donor in the higher aggregates. In all aggregates the shortest-lived component, ranging from 50 ps for monomer to 10 ps for hexamers, is observed as a decay term (positive amplitude) at short emission wavelength. At long emission wavelength it turns into a rise term (negative amplitude). The lifetime of a second ps-component ranges from 200 ps for monomers to 50 ps for hexamers. The long-lived (ns) fluorescence is inhomogeneous in monomers and trimers, showing two lifetimes of ~0.6 and 1.3 ns. The latter one carries the larger amplitude. The amplitudes of the kinetic components in the fluorescence decays are presented as time-resolved component spectra. A theoretical model has been derived to rationalize the observed fluorescence kinetics. Using symmetry arguments, it is shown that the fluorescence kinetics of C-Phycocyanin is expected to be characterized by three exponential kinetic components, independent of the aggregation state. An analytical expression is derived, which allows us to gain a detailed understanding of the origin of the different kinetic components and their associated time-resolved spectra. Numerical calculations of time-resolved spectra are compared with the experimental data.