Fluorescence decay kinetics of chlorophyll in photosynthetic membranes

The absorption of light by the pigments of photosynthetic organisms results in electronic excitation that provides the energy to drive the energy-storing light reactions. A small fraction of this excitation gives rise to fluorescence emission, which serves as a sensitive probe of the energetics and kinetics of the excited states. The wavelength dependence of the excitation and emission spectra can be used to characterize the nature of the absorbing and fluorescing molecules and to monitor the process of sensitization of the excitation transfer from one pigment to another. This excitation transfer process can also be followed by the progressive depolarization of the emitted radiation. Using time-resolved fluorescence rise and decay kinetics, measurements of these processes can now be characterized to as short as a few picoseconds. Typically, excitation transfer among the antenna or light harvesting pigments occurs within 100 psec, whereupon the excitation has reached a photosynthetic reaction center capable of initiating electron transport. When this trap is functional and capable of charge separation, the fluorescence intensity is quenched and only rapidly decaying kinetic components resulting from the loss of excitation in transit in the antenna pigment bed are observed. When the reaction centers are blocked or saturated by high light intensities, the photochemical quenching is relieved, the fluorescence intensity rises severalfold, and an additional slower decay component appears and eventually dominates the decay kinetics. This slower (1-2 nsec) decay results from initial charge separation followed by recombination in the blocked reaction centers and repopulation of the excited electronic state, leading to a rapid delayed fluorescence component that is the origin of variable fluorescence. Recent growth in the literature in this area is reviewed here, with an emphasis on new information obtained on excitation transfer, trapping, and communication between different portions of the photosynthetic membranes.     

Characterization of long-range electron transfer in mixed-metal [zinc,iron] hybrid hemoglobins

Measurements characterizing electron transfer from a photoexcited zinc protoporphyrin triplet (3ZnP) to a ferriheme electron acceptor within the [alpha 1,beta 2] electron-transfer complex of [FeIII,Zn] hybrid hemoglobins are reported. Analytical results demonstrate that the hybrids studied are pure, homogeneous proteins with 1:1 ZnP:FeP content. Within the T quaternary structure adopted by these hybrids, the optical spectrum of a FeIIIP is perturbed by the protein environment. Room temperature kinetic studies of the rate of 3ZnP decay as a function of the heme oxidation and ligation state demonstrate that quenching of 3ZnP by FeIII(H2O)P occurs by long-range intramolecular electron transfer with rate constant kt = 100 (+/- 10) s-1 and is not complicated by spin-quenching or energy-transfer processes; results are the same for alpha(Zn) and beta(Zn) hybrids. Replacement of H2O as a ligand to the ferriheme changes the 3ZnP----FeIIIP electron-transfer rate constant, kt, which demonstrates that electron transfer, not conformational conversion, is rate limiting. However, the trend is not readily explained by simple considerations of spin-state and bonding geometry: kt decreases in the order imidazole greater than H2O greater than F- approximately CN- approximately N3-. The reverse electron-transfer process FeIIP----ZnP+ has not been observed directly but has been shown to be much more rapid, with rate constant kb greater than 10(3) s-1, consistent with the possible importance of "hole" superexchange in electron tunneling within protein complexes.     

Interaction of flavin adenine dinucleotide (FAD) with a glassy carbon electrode surface

The interaction of flavin adenine dinucleotide (FAD) with a glassy carbon electrode (GCE) surface was investigated in terms of the FAD adsorption thermodynamics and kinetics, the subsequent electroreduction mechanism, and the corresponding electron-transfer rate. The kinetics of FAD electroreduction at the GCE was found to be an adsorption-controlled process. A set of electroreduction kinetic parameters was calculated: the true number of electrons involved in the FAD reduction, n=1.76, the apparent transfer coefficient, alpha(app)=0.41, and the apparent heterogeneous electron-transfer rate constant, k(app)=1.4 s(-1). The deviation of the number of exchanged electrons from the theoretical value for the complete reduction of FAD to FADH(2) (n=2) indicates that a small portion of FAD goes to a semiquinone state during the redox process. The FAD adsorption was well described by the Langmuir adsorption isotherm. The large negative apparent Gibbs energy of adsorption (DeltaG(ads)=-39.7 +/-0.4 kJ mol(-1)) indicated a highly spontaneous and strong adsorption of FAD on the GCE. The energetics of the adsorption process was found to be independent of the electrode surface charge in the electrochemical double-layer region. The kinetics of FAD adsorption was modeled using a pseudo-first-order kinetic model.     

Photo-induced electron transfer between hypocrellins and nano-sized semiconductor CdS-- EPR study on the kinetics of photosensitized reduction in HA-CdS and HB-CdS systems

Both HA-CdS and HB-CdS (Hys-CdS, Hys represents HA, HB) complex systems were established according to the dynamics of heterogeneous electron-transfer process ＜0. In these systems, the electron transferring from 1Hys* to conduction band of CdS is feasible. Determined from the fluorescence quenching, the apparent association constants (Kapp) between Hypocrellin A (HA), Hypocrellin B (HB) and CdS sol. were about 940 (mol/L)-1, 934 (mol/L)-1, respectively. Fluorescence lifetime measurements gave the rate constant for the electron transfer process from 1HA*, 1HB* into conduction band of CdS semiconductor as 5.16×109 s-1, 5.10×109 s-1, respectively. TEMPO (2,2,6,6-tetramethy-1-piperdinyloxy), a stable nitroxide radical, was used in the kinetic study of the reduction reaction taking place on the surface of a CdS colloidal semiconductor, kinetics equation of the reaction was determined with the electron paramagnetic resonance (EPR) method, and the reaction order of TEMPO is zero. When Hys were added, the rate of EPR increased greatly. By comparing rate constants, the Hys-CdS systems were revealed to be about 350 times more efficient than CdS sol. alone in the photoreduction of TEMPO under visi-ble light. It suggests that Hys can be used as efficient sensitizers of a colloidal semiconductor in the application of solar energy.     

Structure-based kinetic modeling of excited-state transfer and trapping in histidine-tagged photosystem II core complexes from synechocystis

Chlorophyll fluorescence decay kinetics in photosynthesis are dependent on processes of excitation energy transfer, charge separation, and electron transfer in photosystem II (PSII). The interpretation of fluorescence decay kinetics and their accurate simulation by an appropriate kinetic model is highly dependent upon assumptions made concerning the homogeneity and activity of PSII preparations. While relatively simple kinetic models assuming sample heterogeneity have been used to model fluorescence decay in oxygen-evolving PSII core complexes, more complex models have been applied to the electron transport impaired but more highly purified D1-D2-cyt b(559) preparations. To gain more insight into the excited-state dynamics of PSII and to characterize the origins of multicomponent fluorescence decay, we modeled the emission kinetics of purified highly active His-tagged PSII core complexes with structure-based kinetic models. The fluorescence decay kinetics of PSII complexes contained a minimum of three exponential decay components at F(0) and four components at F(m). These kinetics were not described well with the single radical pair energy level model, and the introduction of either static disorder or a dynamic relaxation of the radical pair energy level was required to simulate the fluorescence decay adequately. An unreasonably low yield of charge stabilization and wide distribution of energy levels was required for the static disorder model, and we found the assumption of dynamic relaxation of the primary radical pair to be more suitable. Comparison modeling of the fluorescence decay kinetics from PSII core complexes and D1-D2-cyt b(559) reaction centers indicated that the rates of charge separation and relaxation of the radical pair are likely altered in isolated reaction centers.     

Effective lattice behavior of fluorescence energy transfer at lamellar macromolecular interfaces.

Fluorescence energy transfer between donors and acceptors confined to macromolecular interfaces is considered. In particular, we discuss two theoretical models for the ensemble-average fluorescence intensity decay of the donor when both fluorophores are incorporated into a planar (e.g., lamellar) interface. The first model is based on a continuous distribution of donor and acceptor molecules on a two-dimensional surface, whereas the other assumes a discrete distribution of fluorophores along the nodes of a two-dimensional square lattice. Results for the discrete model show that the fluorescence intensity kinetics of a donor depends strongly on the geometry of the molecular distribution (i.e., the lattice constant) and the photophysics of fluorophores (i.e., critical radius of the energy transfer). Furthermore, a "discrete molecular distribution" might manifest itself in the experimental data as an increase in the apparent dimensionality of the energy transfer with increasing acceptor concentration. Altogether, the experimental and theoretical underpinnings indicate the enormous potential of using fluorescence energy-transfer kinetics for revealing structural features of molecular ensembles (i.e., geometry, shape) based on a single experimental measurement. However, further understanding the effects of restricted geometries on the fluorescence energy transfer is required to take full advantage of this information. Basic theoretical considerations to that end are provided.     

基于电子回流理论的植物延迟荧光来源理论与实验研究

延迟荧光(DF)技术在植物学、农业和环境等领域有着广泛的应用前景,延迟荧光来源的机理研究对其应用起着重要的作用。基于广泛接受的电子回流理论由一系列的光化学反应方程推导得出多指数衰减的延迟荧光动力学模型,首次提出了一个简化的三指数衰减近似模型,描述了光合电子传递链上的三个最重要成分的电子回流。为了验证近似模型的准确性,以实验室培养的相似的8周大的Jin Dan No.39玉米叶片为模型样品,利用实验室自制的延迟荧光探测系统,得到延迟荧光衰减动力学曲线。分别用三种电子阻断剂:DCMU、DB-MIB和Paraquat处理后的衰减动力学的实验与理论模型进行了对比研究,通过曲线特征来确定不同成分的存在及依赖关系。结果表明延迟荧光衰减动力学三指数拟合非常好(R2=0.99909),而且这三种成分是相互独立的,分别来源于QA,QB和光系统Ⅰ环式电子流。简化模型的提出为延迟荧光的应用题提供一个平台。     

Delayed fluorescence from Rhodopseudomonas viridis following single flashes.

Delayed fluorescence from Rhodopseudomonas viridis membrane fragments has been studies using a phosphoroscope employing single, short actinic flashes, under conditions of controlled redox potential and temperature. The emission spectrum shows that delayed fluorescence is emitted by the bulk, antenna bacteriochlorophyll. The energy for delayed fluorescence, however, must be stored in a reaction-center complex including the photooxidized form (P+) of the primary electron-donor (P) and the photoreduced form (X MINUS) of the primary electron-acceptor. This is shown by the following observations: (1) Delayed luminescence is quenched (a) at low redox potentials which allow cytochromes to reduce P+ rapidly after the flash, (b) at higher redox potentials which, by oxidizing P chemically, prevent the photochemical formation of P+X minus, and (c) upon transfer of an electron from X minus to a secondary acceptor, Y. (2) Under conditions that prevent the reduction of P+ by cytochromes and the oxidation of X minus by Y, the decay kinetics of delayed fluorescence are identical with those of P+X minus, as measured from optical absorbance changes. The main decay route for P+X minus under these conditions has a rate-constant of approximately 10-3-s-minus 1. In contrase, a comparison of the intensities of delayed and prompt fluorescence indicates that the process in which P+X minus returns energy to the bulk bacteriochlorophyll has a rate-constant of 3.7 s-minus 1, at 295 degrees K and pH 7.8. The decay kinetics of P+X minus and delayed fluorescence change little with temperature, whereas the intensity of delayed fluorescence increases with increasing temperature, having an activation energy of 12.5 kcal mol-mol- minus 1. We conclude that the main decay route involves tunneling of an electron from X minus to P+, without the promotion of P to an excited state. Delayed fluorescence requires such a promotion, followed by transfer of energy to the bulk bacteriochlorophyll, and this combination of events is rare. The activation energy, taken with potentiometric data, indicates that the photochemical conversion of PX to P+X minus results in increases of both the energy and the entropy of the system, by 16.6 kcal-mol- minus 1 and 8.8 cal-mol- minus 1-deg- minus 1. The intensity of delayed fluorescence depends strongly on the pH; the origin of this effect remains unclear.     

Direct voltammetric investigation of the electrochemical properties of human hemoglobin: relevance to physiological redox chemistry

Voltammetric measurements on solutions of human hemoglobin using gold electrodes modified with omega-hydroxyalkanethiols have yielded the first direct measure of the reorganization energy of the protein. The value obtained based on extrapolation of the experimentally measured currents, 0.76 eV, is independent of pH (i.e., over the physiologically relevant rage, pH 6.8-7.4) and is remarkably similar to values obtained for myoglobin. This result is perhaps surprising given the marked dependence of the measured reduction potential of hemoglobin on pH (i.e., the redox Bohr effect). Electron transfer rates from the electrode to hemoglobin were also measured. Using similarly measured heterogeneous electron-transfer rates for cytochrome b(5), it is possible to predict the magnitude of the homogeneous electron-transfer rate from cytochrome b(5) to methemoglobin using a formalism developed by Marcus. These predicted rates are in reasonable agreement with reported rates of this physiological reaction based on stopped-flow kinetics experiments. These results suggest that the intrinsic electroreactivity of these heme proteins is sufficient to account for physiologically observed rates. Residual differences between homogeneous phase kinetics and those predicted by heterogeneous phase reactions are suggested to be due to small reductions in the outer-sphere reorganization energy of both component proteins which arise due to solvent exclusion at the interface between the two proteins in complex.     

Electron transfer from quinohemoprotein alcohol dehydrogenase to blue copper protein azurin in the alcohol oxidase respiratory chain of Pseudomonas putida HK5.

A blue copper protein was purified together with a type II quinohemoprotein alcohol dehydrogenase (ADH IIB) from the soluble fraction of Pseudomonas putida HK5 grown on n-butanol. The purified blue copper protein was shown to be azurin, on the basis of several properties such as its absorption maximum (623 nm), its low molecular mass (17 500 Da), its acidic nature (pI of 4.1), its relatively high redox potential (306 mV), the presence of an intramolecular disulfide bond, and N-terminal amino acid sequence homology with respect to azurins from other sources, especially from P. putida NCIB 9869 and Pseudomonas fluorescens. Direct electron transfer from ADH IIB to azurin was shown to occur at a rate of 48-70 s-1. The apparent Km value of ADH IIB for azurin, determined by steady-state kinetics, was decreased several-fold by increasing the ionic strength. Furthermore, the extent of fluorescence quenching of ADH IIB due to the interaction with azurin was increased by increasing the ionic strength, but the binding constant for binding between ADH IIB and azurin was unchanged. The redox potential of azurin was increased 12 mV by incubation with ADH but not vice versa. Furthermore, the redox potential gap between ADH and azurin was increased from 102 to 126 mV by increasing the ionic strength. It is conceivable that a hydrophobic interaction is involved in the electron transfer between both proteins, and it is also suggested that the electron transfer may occur by a freely reversible on and off binding process but may not be related to the global binding process of both proteins. Thus, the results presented here strongly suggest that azurin works as an electron-transfer mediator in a PQQ-dependent alcohol oxidase respiratory chain in P. putida HK5.     

Study of electron transport in heme proteins. X. Effect of pH, ionic strength, and zinc ions and the rate of ferricytochrome c reduction by oxymyoglobin from swine heart]

The rate of the redox reaction between porcine MbO2 and ferri-Cyt c at different ionic strengths in the pH range 5-8 has been studied. At low ionic strength (I = 0-0.1) the pH dependence curve was found to have a sigmoid shape with pKeff approximately 5.7, implying the effect of ionization of His-119(GH1) at the "active site" of myoglobin on the kinetics of the process. In this range of ionic strengths the rate of the reaction decreases sharply. The slope of the curve in the coordinates of IgKexp versus square root of I/1 + square root of I varies depending on pH. It is greater at pH less than or equal to 6 and smaller at pH 7.5, which is due to deprotonation of His(GH1). At high ionic strength (I greater than 0.1) the rate of electron transfer is negligible, independent of pH and does not practically change as I increases from 0.1 to 1. It is shown that the local electrostatic interactions play a decisive role in the formation of an efficient electron-transfer complex between Mb and Cyt c. The binding of the zinc ion to His(GH1) was found to inhibit the electron transfer at I = 0.01, similarly to what occurs at a high ionic strength, though the "reactive" charges of the proteins are not screened and the positive charge at His(GH1) is retained. This suggests that His(GH1) is directly involved in the mechanism of electron transfer from Mb to Cyt c. The data obtained are compared with earlier data on the effect of pH, ionic strength and zinc ions on the reaction between MbO2 from sperm whale and Cyt c. To explain the higher efficiency of pig MbO2 as electron donor, the electrostatic and steric properties of both myoglobins have been analyzed.     

Picosecond time-resolved fluorescence studies on excitation energy transfer in a histidine 117 mutant of the D2 protein of photosystem II in Synechocystis 6803

The role of the peripheral reaction center chlorophyll a molecule associated with His117 of the D2 polypeptide in photosystem II was investigated in Synechocystis sp. PCC 6803 using a combination of steady state, pump-probe, and picosecond time-resolved fluorescence spectroscopy. Data were obtained from intact cells and isolated thylakoid membranes of a control mutant and a D2-H117T mutant, both of which lacked photosystem I. Excitation energy transfer and trapping were investigated by analyzing the data with a kinetic model that used an exact numerical solution of the Pauli master equation, taking into account available photosystem II spectral and structural information. The results of our kinetic analysis revealed the observed difference in excited-state dynamics between the H117T mutant and the control to be consistent with a retardation of the rate of excitation energy transfer from the peripheral chlorophyll of D2 (Chl at His117) to the electron-transfer pigments and an increase of the rate constant for charge recombination in the H117T mutant. The kinetic model was able to account for the experimentally observed changes in absorption cross section and fluorescence decay kinetics between the control and mutant by invoking changes in only these two rate constants. The results rule out quenching of excitation by a chlorophyll cation radical as a mechanism responsible for the lower efficiency of excitation energy utilization in the H117T mutant. Our work also demonstrates the importance of the chlorophyll associated with His117 of the D2 protein for excitation energy transfer to the PSII electron-transfer pigments and for the effective stabilization of the primary radical pair.     

Energy transfer in photosystem I of cyanobacteria Synechococcus elongatus: model study with structure-based semi-empirical Hamiltonian and experimental spectral density

We model the energy transfer and trapping kinetics in PSI. Rather than simply applying F?rster theory, we develop a new approach to self-consistently describe energy transfer in a complex with heterogeneous couplings. Experimentally determined spectral densities are employed to calculate the energy transfer rates. The absorption spectrum and fluorescence decay time components of the complex at room temperature were reasonably reproduced. The roles of the special chlorophylls (red, linker, and reaction center, respectively) molecules are discussed. A formally exact expression for the trapping time is derived in terms of the intrinsic trapping time, mean first passage time to trap, and detrapping time. The energy transfer mechanism is discussed and the slowest steps of the arrival at the primary electron donor are found to contain two dominant steps: transfer-to-reaction-center, and transfer-to-trap-from-reaction-center. The intrinsic charge transfer time is estimated to be 0.8 approximately 1.7 ps. The optimality with respect to the trapping time of the calculated transition energies and the orientation of Chls is discussed.     

Spectral heterogeneity and time-resolved spectroscopy of excitation energy transfer in membranes of Heliobacillus mobilis at low temperatures.

Transient absorption difference spectra in the Qy absorption band from membranes of Heliobacillus mobilis were recorded at 140 and 20 K upon 200 fs laser pulse excitation at 590 nm. Excitation transfer from short wavelength absorbing forms of bacteriochlorophyll g to long wavelength bacteriochlorophyll g occurred within 1-2 ps at both long wavelength bacteriochlorophyll g occurred within 1-2 ps at both temperatures. In addition, a slower energy transfer process with a time constant of 15 ps was observed at 20 K within the pool of long wavelength-absorbing bacteriochlorophyll g. Energy transfer from long wavelength antenna pigments to the primary electron donor P798 was observed, yielding the primary charge-separated state P798+A0-. The time constant for this process was 30 ps at 140 K and about 70 ps at 20 K. A decay component with smaller amplitude and a lifetime of up to hundreds of picoseconds was observed that was centered around 814 nm at 20 K. Kinetic simulations using simple lattice models reproduce the observed decay kinetics at 295 and 140 K, but not at 20 K. The kinetics of energy redistribution within the spectrally heterogeneous antenna system at low temperature argue against a simple "funnel" model for the organization of the antenna of Heliobacillus mobilis and favor a more random spatial distribution of spectral forms. However, the relatively high rate of energy transfer from long wavelength antenna bacteriochlorophyll g to the primary electron donor P798 at low temperature is difficult to explain with either of these models.     

Time-resolved fluorescence analysis of the recombinant photosystem II antenna complex CP29. Effects of zeaxanthin, pH and phosphorylation.

Nonradiative dissipation of excitation energy is the major photoprotective mechanism in plants. The formation of zeaxanthin in the antenna of photosystem II has been shown to correlate with the onset of nonphotochemical quenching in vivo. We have used recombinant CP29 protein, over-expressed in Escherichia coli and refolded in vitro with purified pigments, to obtain a protein indistinguishable from the native complex extracted from thylakoids, binding either violaxanthin or zeaxanthin together with lutein. These recombinant proteins and the native CP29 were used to measure steady-state chlorophyll fluorescence emission and fluorescence decay kinetics. We found that the presence of zeaxanthin bound to CP29 induces a approximately 35% decrease in fluorescence yield with respect to the control proteins (the native and zeaxanthin-free reconstituted proteins). Fluorescence decay kinetics showed that four components are always present but lifetimes (tau) as well as relative fluorescence quantum yields (rfqy) of the two long-lived components (tau3 and tau4) are modified by the presence of zeaxanthin. The most relevant changes are observed in the rfqy of tau3 and in the average lifetime ( approximately 2.4 ns with zeaxanthin and 3.2-3.4 ns in the control proteins). When studied in vitro, no significant effect of acidic pH (5.2-5.3) is observed on chlorophyll A fluorescence yield or kinetics. The data presented show that recombinant CP29 is able to bind zeaxanthin and this protein-bound zeaxanthin induces a significant quenching effect.     

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.     

Properties of the proteinaceous component acting as apoenzyme for the functional plastoquinone redox groups on the acceptor side of system II

The electron-transfer reactions between the plastoquinone molecules of the acceptor side of photosystem II have been inferred to be regulated by a proteinaceous component (apoenzyme), which additionally contains the receptor site for DCMU-type inhibitors (Renger, G., (1976) Biochim. Biophys. Acta 440, 287–300). In order to reveal the functional properties of this apoenzyme, the effect of procedures which modify the structure of proteins on the photosystem II electron transport have been investigated in isolated spinach chloroplasts by comparative measurements of O₂ evolution and absorption changes at 334 nm induced by repetitive flash excitation and of fluorescence induction curves caused by continuous actinic light. It was found that: (1) The release of blockage of O₂ evolution by the DCMU-type inhibitor SN 58132 due to mild tryptic digestion correlates kinetically with the deterioration of the binding properties. (2) Glutaraldehyde fixation of chloroplasts does not markedly modify the reoxidation kinetics of the reduced primary plastoquinone acceptor component, X320^?, of photosystem II, but it greatly reduces the fluorescence yield of the antenna chlorophylls and slightly retards the ADRY effect. Furthermore, it prevents the attack of trypsin on the apoenzyme. (3) Incubation of chloroplasts in ‘low’ salt medium markedly diminishes the ability of trypsin to release the blockage of O₂ evolution by SN 58132 and completely presents the effect on inhibition by DCMU. Based on these results and taking into account recent findings of other groups, the functional mechanism of the electron transport on the acceptor side of photosystem II is discussed. Assuming a tunnel mechanism, the apoprotein is inferred to act as a dynamic regulator rather than changing only the relative levels of the redox potentials of the plastoquinone molecules involved in the transfer steps. It is further concluded that salt depletion does not only cause grana unstacking and a change of the excitation energy transfer probabilities, but it additionally modifies the orientation of functional membrane proteins of photosystem II and their structural interaction within the thylakoid membrane.     

Transient kinetics of redox reactions of flavodoxin: effects of chemical modification of the flavin mononucleotide prosthetic group on the dynamics of intermediate complex formation and electron transfer

The effects of structural modifications of the flavin mononucleotide (FMN) prosthetic group of Clostridium pasteurianum flavodoxin on the kinetics of electron transfer to the oxidized form (from 5-deazariboflavin semiquinone produced by laser flash photolysis) and from the semiquinone form (to horse heart cytochrome c by using stopped-flow spectrophotometry) have been investigated. The analogues used were 7,8-dichloro-FMN, 8-chloro-FMN, 7-chloro-FMN, and 5,6,7,8-tetrahydro-FMN. The ionic strength dependence of cytochrome c reduction was not affected by chlorine substitution, although the specific rate constants for complex formation and decay were appreciably smaller. On the other hand, all of the chlorine analogues had the same rate constant for deazariboflavin semiquinone oxidation. The rate constants for tetrahydro-FMN flavodoxin semiquinone reduction of cytochrome c were considerably smaller than those for the native protein. The implications of these results for the electron-transfer mechanism of flavodoxin are discussed.     

Fluorescence induction in the phycobilisome-containing cyanobacterium Synechococcus sp PCC 7942: analysis of the slow fluorescence transient

At room temperature, the chlorophyll (Chl) a fluorescence induction (FI) kinetics of plants, algae and cyanobacteria go through two maxima, P at approximately 0.2-1 and M at approximately 100-500 s, with a minimum S at approximately 2-10 s in between. Thus, the whole FI kinetic pattern comprises a fast OPS transient (with O denoting origin) and a slower SMT transient (with T denoting terminal state). Here, we examined the phenomenology and the etiology of the SMT transient of the phycobilisome (PBS)-containing cyanobacterium Synechococcus sp PCC 7942 by modifying PBS-->Photosystem (PS) II excitation transfer indirectly, either by blocking or by maximizing the PBS-->PS I excitation transfer. Blocking the PBS-->PS I excitation transfer route with N-ethyl-maleimide [NEM; A. N. Glazer, Y. Gindt, C. F. Chan, and K.Sauer, Photosynth. Research 40 (1994) 167-173] increases both the PBS excitation share of PS II and Chl a fluorescence. Maximizing it, on the other hand, by suspending cyanobacterial cells in hyper-osmotic media [G. C. Papageorgiou, A. Alygizaki-Zorba, Biochim. Biophys. Acta 1335 (1997) 1-4] diminishes both the PBS excitation share of PS II and Chl a fluorescence. Here, we show for the first time that, in either case, the slow SMT transient of FI disappears and is replaced by continuous P-->T fluorescence decay, reminiscent of the typical P-->T fluorescence decay of higher plants and algae. A similar P-->T decay was also displayed by DCMU-treated Synechococcus cells at 2 degrees C. To interpret this phenomenology, we assume that after dark adaptation cyanobacteria exist in a low fluorescence state (state 2) and transit to a high fluorescence state (state 1) when, upon light acclimation, PS I is forced to run faster than PS II. In these organisms, a state 2-->1 fluorescence increase plus electron transport-dependent dequenching processes dominate the SM rise and maximal fluorescence output is at M which lies above the P maximum of the fast FI transient. In contrast, dark-adapted plants and algae exist in state 1 and upon illumination they display an extended P-->T decay that sometimes is interrupted by a shallow SMT transient, with M below P. This decay is dominated by a state 1-->2 fluorescence lowering, as well as by electron transport-dependent quenching processes. When the regulation of the PBS-->PS I electronic excitation transfer is eliminated (as for example in hyper-osmotic suspensions, after NEM treatment and at low temperature), the FI pattern of Synechococcus becomes plant-like.