Effect of cations on the quantum yield and the lifetime of the chloroplast fluorescence]

The interrelationship between the cation-induced fluorescence changes and the state of the photosystem 2 (PS-2) reaction centers for pea chloroplasts and their osmotic fragments was studied. The effects of K+ and Mg2+ on the fluorescence quantum yield (phi f1) under varying light intensities as well as on the fluorescence lifetime (tau f1) in the saturating light were demonstrated. K+ induces the decrease in tau f1; Mg2+ exerts an opposite effect. The effects were more pronounced when the reaction centers of PS-2 were converted into an inactive state by illuminating the sample with a saturating light or by adding DCMU. Under these conditions the cations' effect on tau f1 was accompanied by proportional changes in tau f1. It was concluded that in Mg-deficient chloroplasts an efficient channel of the excitation quenching appears in antenna chlorophyll of PS-2 with the rate constant of 7 . 10(8) s-1. The simultaneous measurements of tau f1 by phase and modulation type techniques allowed to reveal the emission heterogeneity within the nanosecond time interval and the DCMU-sensitive delayed fluorescence with the lifetime exceeding 10(-7) s and the overall quantum yield approximately equal to 2 . 10(-3).     

Effects of relaxation processes on the temperature dependence of oxidation rate of photooxidized bacteriochlorophyll on the primary quinone in reaction centers of Rhodobacter sphaeroides

The temperature dependence of the time of dark recombination of charges between photooxidized bacteriochlorophyll and reduced primary quinone acceptor (tau e) in Rhodobacter sphaeroides photosynthetic reaction centers was studied in the temperature range 140-320 K. It was found that the function tau e = tau e(T) is nonmonotonous: in the temperature range from 140 to 290 K, tau e is increased from 40 to 100 ms; however, under further heating to 320 K, tau e decreased to 80 ms. The replacement of H2O by D2O in these preparations caused an acceleration of the recombination process in the range of physiological temperatures, but the nonmonotonous character of the function tau e(T) remained. The theoretical interpretation of the results was made in the framework of the theory of electron-phonon interactions with allowance for the relaxation processes.     

Two-dimensional electron transfer from cytochrome C to photosynthetic reaction centers

The arrangement and the electron transfer are studied for photosynthetic reaction centers (RC) of Rhodopseudomonas sphaeroides reconstituted into phospholipid vesicles. Freeze-etch electron micrographs of phase separated mixed vesicles reveal an RC enrichment in the phase containing the acidic lipid serine. It is demonstrated that the electron transfer from cytochrome c to RC involves a two-dimensional diffusion of the membrane bound electron donor with diffusion coefficients (D approximately 10(-9) cm2/sec) characteristic for membrane proteins.     

Methods of physical labels--a combined approach to the study of microstructure and dynamics in biological systems

The physical principles of several new approaches to the investigation of biological and model systems are discussed, including versions of the spin label method based on relaxation measurements, and also the methods of triplet, M?ssbauer, electron-scattering and radical-pair labels and probes. It is shown that all these methods make it possible to investigate molecular mobility of the medium with the correlation frequencies tau c-1 = 10(-3) -10(11) s-1, to measure the rate constants of collisions Ktr = 10(3) -10(10) M-1 s-1, to measure the distance between centers up to 100 A and finally, to evaluate the immersion depths of paramagnetic and chromophore centers in matrices up to 40 A. The combined approach is demonstrated with examples from studies of the structure of nitrogenase, the reaction centers of photosynthetic bacteria and sarcoplasmic reticulum membranes and from studies of the molecular dynamics of proteins and membranes.     

Possible effect of structural phase transition in the reactive center of Rhodobacter sphaeroides on the rate of dark adaptation of photooxidized bacteriochlorophyll from primary quinone

The dependence of the rate of dark recombination between the photooxidized primary donor--dimer bacteriochlorophyll molecule (P) and reduced primary quinone acceptor (QA), P+QA(-)-->PQA was studied in photosynthetic reaction centers (RC) from Rhodobacter sphaeroides in the temperature range of 100-320 K. Control RC preparations, RC species with the removed H-subunit as well as RC samples with the hydrogen bonds network modified by isotopic D2O-H2O substitution were investigated. An anomalous temperature dependence of the recombination time (tau rec) of dark reaction P+QA(-)-->PQA was found for all RC samples. It was found that upon heating from 120 to 290 K tau rec increased 2.5 fold. However, upon further heating to 320 K, tau rec decreased again. The temperature dependences of the P+QA(-)-->PQA recombination time were compared with those of the thermodepolarization current of RC preparations in the same temperature range. The temperature curve of the thermodepolarization current was also nonmonotonous. The theoretical interpretation of the temperature dependence of tau rec as well as of the thermodepolarization current was made in the framework of the theory of structural phase transitions within the hydrogen bond network in the water-protein surrounding of the redox centers participating in the electron transfer reactions.     

Electrochromic detection of a coherent component in the formation of the charge pair P(+)H(L)(-) in bacterial reaction centers

We demonstrate coupling of an intraprotein electron transfer reaction to coherent vibrational motions. The kinetics of charge separation toward the radical pair state P(+)H(L)(-) were studied in reaction centers of Rhodobacter sphaeroides at 15 K. The electrochromic shift of the bacteriochlorophyll monomers is the most prominent spectral feature associated with this charge displacement. The newly reported absolute absorption spectrum of the P(+)H(L)(-) state is discussed in terms of this shift. In wild-type reaction centers, the rise kinetics of the electrochromic shift display a small but significant 30 cm(-)(1) periodic modulation (period of approximately 1 ps). This modulation is also present in FL181Y mutant reaction centers, where overall charge separation is somewhat more rapid than in the wild-type reaction center. In contrast, in YM210L mutant reaction centers, where the charge separation is much slower, the modulation is absent. The conclusion that the motion along the reaction coordinate has a 30 cm(-)(1) coherent component is discussed in light of possible mechanisms of electron transfer.     

-deltaG(AB) and pH dependence of the electron transfer from P(+)Q(A)(-)Q(B) toP(+)Q(A)Q(B)(-) in Rhodobacter sphaeroides reaction centers

The electron transfer from the reduced primary quinone (Q(A)(-)) to the secondary quinone (Q(B)) can occur in two phases with a well-characterized 100 micros component (tau(2)) and a faster process occurring in less than 10 micros (tau(1)). The fast reaction is clearly seen when the native ubiquinone-10 at Q(A) is replaced with naphthoquinones. The dependence of tau(1) on the free-energy difference between the P(+)Q(A)(-)Q(B) and P(+)Q(A)Q(B)(-) states (-) and on the pH was measured using naphthoquinones with different electrochemical midpoint potentials as Q(A) in Rhodobacter sphaeroides reaction centers (RCs) and in RCs where - is changed by mutation of M265 in the Q(A) site from Ile to Thr (M265IT). Q(B) was ubiquinone (UQ(B)) in all cases. Electron transfer was measured by using the absorption differences of the naphthosemiquinone at Q(A) and the ubisemiquinone at Q(B) between 390 and 500 nm. As - was changed from -90 to -250 meV tau(1) decreased from 29 to 0.2 micros. The free-energy dependence of tau(1) provides a reorganization energy of 850 +/- 100 meV for the electron transfer from Q(A)(-) to Q(B). The slower reaction at tau(2) is free-energy independent, so processes other than electron transfer determine the observed rate. The fraction of the reaction at tau(1) increases with increasing driving force and is 100% of the reaction when - is approximately 100 meV more favorable than in the native RCs with ubiquinone as Q(A). The fast phase, tau(1), is pH independent from pH 6 to 11 while tau(2) slows above pH 9. As the Q(A) isoprene tail length is increased from 2 to 10 isoprene units the fraction at tau(1) decreases. However, tau(1), tau(2), and the fraction of the reaction in each phase are independent of the tail length of UQ(B).     

Dynamics of energy transfer and trapping in the light-harvesting antenna of Rhodopseudomonas viridis.

By low intensity picosecond absorption spectroscopy it is shown that the exciton lifetime in the light-harvesting antenna of Rhodopseudomonas (Rps.) viridis membranes with photochemically active reaction centers at room temperature is 60 +/- 10 ps. This lifetime reflects the overall trapping rate of the excitation energy by the reaction center. With photochemically inactive reaction centers, in the presence of P+, the exciton lifetime increases to 150 +/- 15 ps. Prereducing the secondary electron acceptor QA does not prevent primary charge separation, but slows it down from 60 to 90 +/- 10 ps. Picosecond kinetics measured at 77 K with inactive reaction centers indicates that the light-harvesting antenna is spectrally homogeneous. Picosecond absorption anisotropy measurements show that energy transfer between identical Bchlb molecules occurs on the subpicosecond time scale. Using these experimental results as input to a random-walk model, results in strict requirements for the antenna-RC coupling. The model analysis prescribes fast trapping (approximately 1 ps) and an approximately 0.5 escape probability from the reaction center, which requires a more tightly coupled RC and antenna, as compared with the Bchla-containing bacteria Rhodospirillum (R.) rubrum and Rhodobacter (Rb.) sphaeroides.     

Ligand binding and the catalytic reaction of cytochrome caa(3) from the thermophilic bacterium Rhodothermus marinus

The ligand-binding dynamics and the reaction with O(2) of the fully (five-electron) reduced cytochrome caa(3) from the thermohalophilic bacterium Rhodothermus (R.) marinus were investigated. The enzyme is a proton pump which has all the residues of the proton-transfer pathways found in the mitochondrial-like enzymes conserved, except for one of the key elements of the D-pathway, the helix-VI glutamate [Glu(I-286), R. sphaeroides numbering]. In contrast to what has been suggested previously as general characteristics of thermophilic enzymes, during formation of the R. marinus caa(3)-CO complex, CO binds weakly to Cu(B), and is rapidly (k(Ba) = 450 s(-1)) trapped by irreversible (K(Ba) = 4.5 x 10(3)) binding to heme a(3). Upon reaction of the fully reduced enzyme with O(2), four kinetic phases were resolved during the first 10 ms after initiation of the reaction. On the basis of a comparison to reactions observed with the bovine enzyme, these phases were attributed to the following transitions between intermediates (pH 7.8, 1 mM O(2)): R --> A (tau congruent with 8 micros), A --> P(r) (tau congruent with 35 micros), P(r) --> F (tau congruent with 240 micros), F --> O (tau congruent with 2.5 ms), where the last two phases were associated with proton uptake from the bulk solution. Oxidation of heme c was observed only during the last two reaction steps. The slower transition times as compared to those observed with the bovine enzyme most likely reflect the replacement of Glu(I-286) of the helix-VI motif -XGHPEV- by a tyrosine in the R. marinus enzyme in the motif -YSHPXV-. The presence of an additional, fifth electron in the enzyme was reflected by two additional kinetic phases with time constants of approximately 20 and approximately 720 ms during which the fifth electron reequilibrated within the enzyme.     

Reaction center and antenna processes in photosynthesis at low temperature

Around 1960 experiments of Arnold and Clayton, Chance and Nishimura and Calvin and coworkers demonstrated that the primary photosynthetic electron transfer processes are not abolished by cooling to cryogenic temperatures. After a brief historical introduction, this review discusses some aspects of electron transfer in bacterial reaction centers and of optical spectroscopy of photosynthetic systems with emphasis on low-temperature experiments.Abbreviations (B)Chl (bacterio)chlorophyll - (B)Phe (bacterio)pheophytin - FMO Fenna-Matthews-Olson - LH1, LH2 light harvesting complexes of purple bacteria - LHC II, CP47 light harvesting complexes of Photosystem II - P, P870 primary electron donor - RC reaction center     

Electron-transfer kinetics in photosynthetic reaction centers cooled to cryogenic temperatures in the charge-separated state: evidence for light-induced structural changes

We have compared the electron-transfer kinetics in reaction centers (RCs) cooled in the dark with those cooled under illumination (i.e., in the charge-separated state). Large differences between the two cases were observed. We interpreted these findings in terms of light-induced structural changes. The kinetics of charge recombination D+QA-----DQA in RCs containing one quinone were modeled in terms of a distribution of donor-acceptor electron-transfer distances. For RCs cooled under illumination the distribution broadened and shifted to larger distances compared to the distribution for RCs cooled in the dark. The model accounts for the nonexponential decay observed at low temperatures [McElroy, J. D., Mauzerall, D. C., & Feher, G. (1974) Biochim. Biophys. Acta 333, 261-277; Morrison, L.E., & Loach, P.A. (1978) Photochem. Photobiol. 27, 751-757]. A possible physiological role of the structural changes is an enhanced charge stabilization. For RCs with two quinones, the recombination kinetics D+QAQB-----DQAQB were found to be strongly temperature dependent. This was interpreted in terms of temperature-dependent transitions between structural states [Agmon, N., & Hopfield, J.J. (1983) J. Chem. Phys. 78, 6947-6959]. This interpretation requires that these transitions occur at cryogenic temperatures on a time scale t greater than or approximately 10(3) s. The electron transfer from QA- to QB was found to not take place in RCs cooled in the dark (tau ABdark greater than 10(-1) s). In RCs cooled under illumination, we found tau ABlight less than 10(-3) s. We suggest the possibility that the drastic decrease in tau AB observed in RCs cooled under illumination is due to the trapping of a proton near QB-.     

Secondary pair charge recombination in photosystem I under strongly reducing conditions: temperature dependence and suggested mechanism.

Photoinduced electron transfer in photosystem I (PS I) proceeds from the excited primary electron donor P700 (a chlorophyll a dimer) via the primary acceptor A0 (chlorophyll a) and the secondary acceptor A1 (phylloquinone) to three [4Fe-4S] clusters, Fx, FA, and FB. Prereduction of the iron-sulfur clusters blocks electron transfer beyond A1. It has been shown previously that, under such conditions, the secondary pair P700+A1- decays by charge recombination with t1/2 approximately 250 ns at room temperature, forming the P700 triplet state (3P700) with a yield exceeding 85%. This reaction is unusual, as the secondary pair in other photosynthetic reaction centers recombines much slower and forms directly the singlet ground state rather than the triplet state of the primary donor. Here we studied the temperature dependence of secondary pair recombination in PS I from the cyanobacterium Synechococcus sp. PCC6803, which had been illuminated in the presence of dithionite at pH 10 to reduce all three iron-sulfur clusters. The reaction P700+A1- --> 3P700 was monitored by flash absorption spectroscopy. With decreasing temperature, the recombination slowed down and the yield of 3P700 decreased. In the range between 303 K and 240 K, the recombination rates could be described by the Arrhenius law with an activation energy of approximately 170 meV. Below 240 K, the temperature dependence became much weaker, and recombination to the singlet ground state became the dominating process. To explain the fast activated recombination to the P700 triplet state, we suggest a mechanism involving efficient singlet to triplet spin evolution in the secondary pair, thermally activated repopulation of the more closely spaced primary pair P700+A0- in a triplet spin configuration, and subsequent fast recombination (intrinsic rate on the order of 10(9) s(-1)) forming 3P700.     

Relaxation kinetics of cytochrome P450 reductase: internal electron transfer is limited by conformational change and regulated by coenzyme binding

The kinetics of internal electron transfer in human cytochrome P450 reductase have been studied using temperature-jump relaxation spectroscopy. Temperature perturbation of CPR reduced at the two-electron level with NADPH yields biphasic absorption transients at 450 and 600 nm. The observed rate, 1/tau, for the fast phase is 2200 +/- 300 s(-1). The absence of this phase in fluorescence transients and in absorption transients collected with dithionite-reduced enzyme indicates this phase does not report on electron/hydride transfer and is consistent with its origin in local conformational change in the vicinity of the FAD isoalloxazine ring. The slow phase (1/tau = 55 +/- 2 s(-1)) observed in the absorption transients obtained with CPR reduced at the two-electron level with NADPH reports on internal electron transfer: FAD(sq)-FMN(sq) --> FAD(ox)-FMN(hq). The observed rate of this transient is slower (1/tau = 11 +/- 0.5 s(-1)) in CPR reduced to the two-electron level by dithionite rather than NADPH, demonstrating that coenzyme binding has an important influence on the observed rate of internal electron transfer. Temperature perturbation experiments with CPR reduced with 10-fold molar excess of NADPH produce monophasic absorption transients (1/tau = 20 +/- 0.2 s(-1)) reporting on internal electron transfer: FAD(sq)-FMN(hq) --> FAD(hq)-FMN(sq). The observed rate constants for electron transfer are substantially less than those expected from analysis of CPR by electron-transfer theory (approximately 10(10) s(-1)). Potential gating mechanisms have been investigated using the temperature-jump method. Observed rates for electron transfer were unaffected in experiments performed in deuterated solvent, indicating that deprotonation does not gate the reaction. Introduction of glycerol into the sample significantly decreased the observed rate for internal electron transfer, suggesting conformational gating of the reaction. Replacement of Trp-676 with His-676 reduces approximately 2-fold the observed rate of internal electron transfer in two-electron-reduced enzyme, whereas the observed rate for FAD(sq)-FMN(hq) --> FAD(hq)-FMN(sq) transfer is increased approximately 13-fold in the W676H mutant reduced with a 10-fold molar excess of NADPH. The studies reveal altered redox properties of the FAD in W676H CPR. The data are discussed in the context of previous stopped-flow studies of human CPR and the X-ray crystallographic structure of rat CPR.     

Charge recombination and protein dynamics in bacterial photosynthetic reaction centers entrapped in a sol-gel matrix

Many proteins can be immobilized in silica hydrogel matrices without compromising their function, making this a suitable technique for biosensor applications. Immobilization will in general affect protein structure and dynamics. To study these effects, we have measured the P(+)Q(A)(-) charge recombination kinetics after laser excitation of Q(B)-depleted wild-type photosynthetic reaction centers from Rhodobacter sphaeroides in a tetramethoxysilane (TMOS) sol-gel matrix and, for comparison, also in cryosolvent. The nonexponential electron transfer kinetics observed between 10 and 300 K were analyzed quantitatively using the spin boson model for the intrinsic temperature dependence of the electron transfer and an adiabatic change of the energy gap and electronic coupling caused by protein motions in response to the altered charge distributions. The analysis reveals similarities and differences in the TMOS-matrix and bulk-solvent samples. In both preparations, electron transfer is coupled to the same spectrum of low frequency phonons. As in bulk solvent, charge-solvating protein motions are present in the TMOS matrix. Large-scale conformational changes are arrested in the hydrogel, as evident from the nonexponential kinetics even at room temperature. The altered dynamics is likely responsible for the observed changes in the electronic coupling matrix element.     

Temperature dependence of electron transfer between bacteriopheophytin and ubiquinone in protonated and deuterated reaction centers of Rhodopseudomonas sphaeroides.

The rate of the electron-transfer reaction between bacteriopheophytin and the first quinone in isolated reaction centers of Rhodopseudomonas sphaeroides has an unusual temperature dependence. The rate increases about threefold with decreasing temperature between 300 and 25 K, and decreases abruptly at temperatures below 25 K. Partial deuteration of the reaction centers alters the temperature dependence of the rate constant. Qualitative features of the temperature dependence can be understood in the context of a theory of nonadiabatic electron transfer (Sarai, 1980. Biochim. Biophys. Acta 589:71-83). We conclude that very low-energy (10-50 cm-1) processes, perhaps skeletal vibrations of the protein, are important to electron transfer. Higher-energy vibrations, possibly involving the pyrrolic N--H bonds of bacteriopheophytin, also are important in this process.     

Calorimetric studies of the kinetic unfreezing of molecular motions in hydrated lysozyme, hemoglobin, and myoglobin.

Differential scanning calorimetric (DSC) studies of the glassy states of as-received and hydrated lysozyme, hemoglobin, and myoglobin powders, with water contents of < or = 0.25, < or = 0.30, and < or = 0.29 g/g of protein, show that their heat capacity slowly increases with increasing temperature, without showing an abrupt increase characteristic of glass-->liquid transition. Annealing (also referred to as physical aging) of the hydrated proteins causes their DSC scans to show an endothermic region, similar to an overshoot, immediately above the annealing temperature. This annealing effect appears at all temperatures between approximately 150 and 300 K. The area under these peaks increases with increasing annealing time at a fixed temperature. The effects are attributed to the presence of a large number of local structures in which macromolecular segments diffuse at different time scales over a broad range. The lowest time scale corresponds to the > N-H and -O-H group motions which become kinetically unfrozen at approximately 150-170 K on heating at a rate of 30 K min-1 and which have a relaxation time of 5-10 s in this temperature range. The annealing effects confirm that the individual glass transition of the relaxing local regions is spread over a temperature range up to the denaturation temperature region of the proteins. The interpretation is supported by simulation of DSC scans in which the distribution of relaxation times is assumed to be exceptionally broad and in which annealing done at several temperatures over a wide range produces endothermic effects (or regions of DSC scans) qualitatively similar to those observed for the hydrated proteins.     

The interaction of quinone and detergent with reaction centers of purple bacteria. I. Slow quinone exchange between reaction center micelles and pure detergent micelles.

The kinetics of light-induced electron transfer in reaction centers (RCs) from the purple photosynthetic bacterium Rhodobacter sphaeroides were studied in the presence of the detergent lauryldimethylamine-N-oxide (LDAO). After the light-induced electron transfer from the primary donor (P) to the acceptor quinone complex, the dark re-reduction of P+ reflects recombination from the reduced acceptor quinones, QA- or QB-. The secondary quinone, QB, which is loosely bound to the RC, determines the rate of this process. Electron transfer to QB slows down the return of the electron to P+, giving rise to a slow phase of the recovery kinetics with time tau P approximately 1 s, whereas charge recombination in RCs lacking QB generates a fast phase with time tau AP approximately 0.1 s. The amount of quinone bound to RC micelles can be reduced by increasing the detergent concentration. The characteristic time of the slow component of P+ dark relaxation, observed at low quinone content per RC micelle (at high detergent concentration), is about 1.2-1.5 s, in sharp contrast to expectations from previous models, according to which the time of the slow component should approach the time of the fast component (about 0.1 s) when the quinone concentration approaches zero. To account for this large discrepancy, a new quantitative approach has been developed to analyze the kinetics of electron transfer in isolated RCs with the following key features: 1) The exchange of quinone between different micelles (RC and detergent micelles) occurs more slowly than electron transfer from QB- to P+; 2) The exchange of quinone between the detergent "phase" and the QB binding site within the same RC micelle is much faster than electron transfer between QA- and P+; 3) The time of the slow component of P+ dark relaxation is determined by (n) > or = 1, the average number of quinones in RC micelles, calculated only for those RC micelles that have at least one quinone per RC (in excess of QA). An analytical function is derived that relates the time of the slow component of P+ relaxation, tau P, and the relative amplitude of the slow phase. This provides a useful means of determining the true equilibrium constant of electron transfer between QA and QB (LAB), and the association equilibrium constant of quinone binding at the QB site (KQ+). We found that LAB = 22 +/- 3 and KQ = 0.6 +/- 0.2 at pH 7.5. The analysis shows that saturation of the QB binding site in detergent-solubilized RCs is difficult to achieve with hydrophobic quinones. This has important implications for the interpretation of apparent dependencies of QB function on environmental parameters (e.g. pH) and on mutational alterations. The model accounts for the effects of detergent and quinone concentration on electron transfer in the acceptor quinone complex, and the conclusions are of general significance for the study of quinone-binding membrane proteins in detergent solutions.     

Temperature- and hydration-dependent protein dynamics in photosystem II of green plants studied by quasielastic neutron scattering

Protein dynamics in hydrated and vacuum-dried photosystem II (PS II) membrane fragments from spinach has been investigated by quasielastic neutron scattering (QENS) in the temperature range between 5 and 300 K. Three distinct temperature ranges can be clearly distinguished by active type(s) of protein dynamics: (A) At low temperatures (T < 120 K), the protein dynamics of both dry and hydrated PS II is characterized by harmonic vibrational motions. (B) In the intermediate temperature range (120 < T < 240 K), the total mean square displacement total slightly deviates from the predicted linear behavior. The QENS data indicate that this deviation, which is virtually independent of the extent of hydration, is due to a partial onset of diffusive protein motions. (C) At temperatures above 240 K, the protein flexibility drastically changes because of the onset of diffusive (large-amplitude) protein motions. This dynamical transition is clearly hydration-dependent since it is strongly suppressed in dry PS II. The thermally activated onset of protein flexibility as monitored by QENS is found to be strictly correlated with the temperature-dependent increase of the electron transport efficiency from Q(A)(-) to QB (Garbers et al. (1998) Biochemistry 37, 11399-11404). Analogously, the freezing of protein mobility by dehydration in dry PS II appears to be responsible for the blockage of Q(A)(-) reoxidation by Q(B) at hydration values lower than 45% r.h. (Kaminskaya et al. (2003) Biochemistry 42, 8119-8132). Similar effects were observed for reactions of the water-oxidizing complex as outlined in the Discussion section.     

Mechanism of Cph1 phytochrome assembly from stopped-flow kinetics and circular dichroism

The kinetics and mechanism of the autocatalytic assembly of holo-Cph1 phytochrome (from Synechocystis) from the apoprotein and the bilin chromophores phycocyanobilin (PCB) and phycoerythrobilin (PEB) were investigated by stopped flow and circular dichroism. At 1:1 stoichiometry, pH 7.9, and 10 degrees C, SVD analysis of the kinetic data for PCB revealed three spectral components involving three transitions with time constants tau(1) approximately 150 ms, tau(2) approximately 2.5 s, and tau(3) approximately 50 s. Tau(1) was associated with a major red shift and transfer of oscillator strength from the Soret region to the 680 nm region. When the sulfhydryl group of cysteine 259 was blocked with iodoacetamide, preventing the formation of a covalent adduct, a noncovalent red-shifted complex (680 nm) was formed with a time constant of 200 ms. Tau(1) could thus be assigned to the formation of a noncovalent complex. The absorption changes during tau(1) are due to the formation of the extended conformation of the linear tetrapyrrole and to its protonation in the binding pocket. From the concentration and pH dependence of the kinetics we obtained a value of 1.5 microM for the K(D) of this noncovalent complex and a value of 8.4 for the pK(a) of the proton donor. The tau(2) component was associated with a blue shift of about 25 nm and was attributed to the formation of the covalent bond (P(r)), accompanied with the loss of the 3-3' double bond to ring A. Tau(3) was due to photoconversion to P(fr). For PEB, which is not photochromic, the formation of the noncovalent complex is faster (tau(1) = 70 ms), but the covalent bond formation is about 80 times slower (tau(2) = 200 s) than with the natural chromophore PCB. The CD spectra of the PCB adduct in the 250-800 nm range show that the chromophore geometries in P(r) and P(fr) are similar to those in plant phytochrome. The opposite rotational strengths of P(r) and P(fr) in the longest wavelength band suggest that the photoisomerization induces a reversal of the chirality. The Cph1 complex with noncovalently bound PCB was still photochromic when cysteine 259 was blocked with IAA or with the bulkier IAF. The covalent linkage to cysteine 259 is thus not required for photoconversion. The CD spectra of the noncovalently bound PCB in P(r)- and P(fr)-like states are qualitatively similar to those of the covalent adducts, suggesting analogous structures in the binding pocket. The noncovalent interactions with the binding pocket are apparently sufficient to hold the chromophore in the appropriate geometry for photoisomerization.     

Sequential assembly of photosynthetic units in Rhodobacter sphaeroides as revealed by fast repetition rate analysis of variable bacteriochlorophyll a fluorescence

The development of functional photosynthetic units in Rhodobacter sphaeroides was followed by near infra-red fast repetition rate (IRFRR) fluorescence measurements that were correlated to absorption spectroscopy, electron microscopy and pigment analyses. To induce the formation of intracytoplasmic membranes (ICM) (greening), cells grown aerobically both in batch culture and in a carbon-limited chemostat were transferred to semiaerobic conditions. In both aerobic cultures, a low level of photosynthetic complexes was observed, which were composed of the reaction center and the LH1 core antenna. Interestingly, in the batch cultures the reaction centers were essentially inactive in forward electron transfer and exhibited low photochemical yields F(V)/F(M), whereas the chemostat culture displayed functional reaction centers with a rather rapid (1-2 ms) electron transfer turnover, as well as a high F(V)/F(M) of approximately 0.8. In both cases, the transfer to semiaerobiosis resulted in rapid induction of bacteriochlorophyll a synthesis that was reflected by both an increase in the number of LH1-reaction center and peripheral LH2 antenna complexes. These studies establish that photosynthetic units are assembled in a sequential manner, where the appearance of the LH1-reaction center cores is followed by the activation of functional electron transfer, and finally by the accumulation of the LH2 complexes.