Trapping, loss and annihilation of excitations in a photosynthetic system. I. Theoretical aspects

In this paper are discussed a few theoretical aspects of the transfer, trapping, loss and annihilation of excitations as they occur in a photosynthetic system after a picosecond light pulse. A random-walk model is introduced to describe the dynamical behavior of the excitations in a domain and is used to calculate the parameter that determines the shape of the total fluorescence yield vs. pulse intensity curve in the case in which the reaction centers are all in the closed state (Paillotin, G., Swenberg, C.E., Breton, J. and Geacintov, N.E. (1979) Biophys. J. 25, 513–533). It is shown that this parameter depends critically on the number, λ, of connected photosynthetic units in a domain. A master equation is postulated to describe the decay of the excitations in the case where the transition of the reaction center from the open to the closed state, induced by the capture of an excitation, is included. The trapping and loss of excitation in a mixture of open and closed reaction centers, generated in the course of the transfer process, is assumed to be described by an equation that is the equivalent for a single domain of the Vredenberg-Duysens relation (Vredenberg, W.J. and Duysens, L.N.M. (1963) Nature 197, 355–357). The master equation is used to find the total probability of loss per excitation, U_λ(z), and the total fraction of reaction centers closed, V_λ(z), as a function of the average number of excitations z created in a domain when the reaction centers are all in the open state before the pulse. It is shown that, for most photosynthetic systems, an increase of U_λ(z) with z can occur only if λ 3. It is further concluded that the combined measurement of U_λ(z) and V_λ(z) can give detailed information about λ and the parameters involved in the transfer process.     

Isolation and amino-terminal sequences of subunits from the photosynthetic reaction center of Rhodopseudomonas capsulata

The amino-terminal sequences have been determined by Edman degradation for the reaction center polypeptides from a carotenoidless mutant of Rhodopseudomonas capsulata. Individual polypeptides were isolated by preparative electrophoresis and electroelution. By comparison with the sequences deduced from the DNA (Youvan, D.C., Alberti, M., Begush, H., Bylina, E.J. and Hearst, J.E. (1984) Proc. Natl. Acad. Sci. USA 81, 189–192) we conclude that the M and L subunits are processed so as to remove the amino-terminal methionine, whereas the H subunit is not processed at the amino-terminus after translation. None of the subunits is synthesized with a significant amino-terminal extension peptide.     

Energetic aspects of photophosphorylation capacity and reaction center content of Rhodopseudomonas capsulata, grown in a turbidostat under different irradiances

Cells of Rhodopseudomonas capsulata were grown in a turbido-stat and adapted to high (1400 W/m²) or low (40 W/m²) light intensities. In high-light-grown cells the specific BChl content was about 10-times lower, the number of intracytoplasmatic membrane vesicles smaller by a factor of about 20, the photosynthetic unit smaller by a factor of 1.9 and the reaction center content about 5-times lower than in low-light-grown cells. However, the photophosphorylation rate per reaction center under saturating light was higher in high-light-grown cells by a factor of 7.7, apparently compensating the lower amount of reaction centers. Adaptation of the cells to different irradiances not only seems to comprise a variation of the size and composition of the antennae, but also a change in the affinity of the photosynthetic system to light, as concluded from saturation curves obtained from the two adaptation stages of cells.     

Fluorescence emission by wild-type- and mutant-strains of Rhodopseudomonas capsulata

Absorption and fluorescence emission spectra of Rhodopseudomonas capsulata, strains 37b4 (wild type), A1a⁺ (blue-green mutant strain), Y5 (phototroph negative, having only B-800–850 bacteriochlorophyll-carotenoid-protein complex) at 4 K, 77 K and 300 K were measured. The fluorescence emission at 890 nm of the B-870 bacteriochlorophyll band dominates the emission of other spectral forms of the strains 37b4 and A1a⁺, while in strain Y5 a fluorescence emission band at 865 nm of the B-850 bacteriochlorophyll dominates. Very little fluorescence was observed at 805 nm. A linear relation between relative fluorescence intensity and the exciting light intensity was observed. The integrated fluorescence yield increased as the temperature was lowered from 300 K to 4 K. The results are discussed in the light of the arrangement of pigment molecules in the membrane and the process of energy migration within the photosynthetic apparatus.     

Evidence for regulation in vivo of the ATP synthase in intact cells of the photosynthetic bacterium Rhodopseudomonas capsulata

(1) The cytoplasmic membrane potential (Δψ) of intact cells of Rhodopseudomonas capsulata, measured either from the uptake of butyltriphenylphosphonium cation or from the electrochromic carotenoid band shift, increased upon illumination (negative on the cytoplasmic side) and then, within the next 20 s, partly declined while the light was still on. In the presence of the F₀ inhibitor venturicidin the light-induced Δψ was increased by 30% and the partial decline was abolished. (2) From the ionic current/Δψ curves for the bacterial membranes it was concluded that the slow, partial decline of Δψ after the onset of illumination was the result of an increase in membrane conductance. The conductance increase seen in the ionic current/Δψ curves was blocked by venturicidin suggesting that it was caused by increased proton flux through the ATP synthase. (3) Analysis of the light-induced changes in adenine nucleotide levels in intact bacterial cells showed that the apparent increase in ATP synthase activity was not the result of a decrease in phosphorylation potential. The data were consistent with either an increase in the catalytic activity of the ATP synthase or with an increase in H⁺ flux through the enzyme without a proportionate increase in the rate of phosphorylation (increased ‘slip’). (4) This slow change in the properties of the ATP synthase, as judged by the venturicidin-sensitive partial decline of Δψ, required a minimum initial value of Δψ. When Δψ was reduced, either by decreasing the actinic light intensity or by adding carbonylcyanide trifluoromethoxyphenylhydrazone the partial decline in Δψ was abolished. (5) The slow change in ATP synthase properties reversed upon darkening the bacterial cell suspension. A second illumination period shortly after the first elicited a smaller initial Δψ and a smaller Δψ decline. The relaxation of the ATP synthase in the dark was measured from the dependence of the initial increase in Δψ after the second illumination period upon the dark-time between the two illumination periods.     

Singlet-singlet annihilation at low temperatures in the antenna of purple bacteria

Chromatophores of the purple photosynthetic bacteria Rhodospirillum rubrum and Rhodobacter (Rhodopseudomonas) sphaeroides were excited by means of 35-ps flashes at 532 nm of varying intensities, both at room temperature and at 4 K. With increasing exciting energy densities the integrated yield of fluorescence produced by these flashes was found to decrease considerably due to singlet-singlet annihilation. An analysis of the results showed that in R. rubrum the number of connected antenna molecules between which energy transfer is possible decreases from about 1000 to about 150 when the temperature is lowered from 298 to 4 K. In Rb. sphaeroides the B875 light-harvesting complex appears to contain about 100 connected bacteriochlorophyll (BChl) 875 molecules at 4 K, while the B800–850 complex contains about 45 BChl 850 molecules. The data are explained by a model for the antenna of Rb. sphaeroides in which units of B875, containing about four reaction centres, are separated by an array of B800–850 units that surrounds B875. By applying a random walk model we found that in both species the rate of energy transfer between neighbouring antenna molecules decreased about 10-fold upon lowering the temperature. The rate of energy transfer from antenna molecules to either open or closed reaction centres decreased only 3- to 4-fold in R. rubrum and remained approximately constant in Rb. sphaeroides upon cooling. A blue shift of the emission spectra at 4 K of both species was observed when the excitation energy density was increased to a level where singlet-singlet annihilation plays a significant role. This observation appears to support the notion that an additional long-wave pigment exists in the antenna of these bacteria.     

Blue and red shifts of bacteriochlorophyll absorption band around 880 nm in Rhodospirillum rubrum

The redox potential dependence of the light-induced absorption changes of bacteriochlorophyll in chromatophores and subchromatophore pigment-protein complexes from Rhodospirillum rubrum has been examined. The highest values of the absorption changes due to the bleaching of P-870 and the blue shift of P-800 in chromatophores and subchromatophore complexes are observed in the 360–410 mV redox potential range. At potentials below 300 mV (pH 7.0), the 880 nm band of bacteriochlorophyll shifts to shorter wavelengths in subchromatophore complexes and to longer wavelengths in chromatophores.

The data on redox titration show that the red and blue shifts of 880-nm bacteriochlorophyll band represent the action of a non-identified component (C₃₄₀) which has an oxidation-reduction midpoint potential close to 340 mV (n = 1) at pH 6.0–7.6. The E_m of this component varies by 60 mV/pH unit between pH 7.6 and 9.2.

The results suggest that the red shift is due to the transmembrane, and the blue shift to the local intramembrane electrical field. The generation of both the transmembrane and local electrical fields is apparently governed by redox transitions of the component C₃₄₀.     

Nucleotide exchange and control of ATPase activity in Rhodospirillum rubrum chromatophores

(1) Light-activated ‘dark’ ATPase in Rhodospirillum rubrum chromatophores is inhibited by preincubation with ADP or ATP (in the absence of Mg²⁺). I₅₀ values were 0.5 and 6 μM, respectively, after 20 s of preincubation. (2) In the absence of MgATP, the rate constant for dissociation of ADP or ATP from the inhibitory site was less than 0.2 min^?1 in deenergized membranes. Illumination in the absence of MgATP caused an increase of over 60-fold in both rate constants. (3) In some experiments hydrolysis was performed in the presence of 10 μM Mg²⁺ and 0.2 mM MgATP. Under these conditions, the ADP or ATP inhibition was reversed within about 20 or about 80 s, respectively, after the onset of hydrolysis. This suggests that recovery from ADP or ATP inhibition (i.e., release of tightly bound ADP or ATP) in the dark is induced by MgATP binding to a second nucleotide-binding site on the enzyme. (4) Results obtained with variable concentrations of uncoupler suggest that in the absence of bound Mg²⁺ (see below), MgATP-induced release of tightly bound ADP or ATP does not require a transmembrane . This, together with the inhibitor/substrate ratios prevalent during hydrolysis, suggests that these reactivation reactions involve MgATP binding to a high-affinity binding site (Kd < 2 μM). (5) At high concentrations of uncoupler, a time-dependent inhibition of hydrolysis occurred in the control chromatophores as well as in the nucleotide-pretreated chromatophores. This deactivation was dependent on Mg²⁺. In addition, MgATP-dependent reversal of ADP inhibition in the dark was inhibited by Mg²⁺ at concentrations above 20–30 μM. By contrast, MgATP-dependent reversal of ADP inhibition occurs within 3–4 s, despite the presence of high concentrations of Mg²⁺ if the chromatophores are illuminated during contact with the nucleotides. Uncoupler abolishes the effect of illumination. A reaction scheme incorporating these findings is proposed. (6) The implications of these findings for the mechanism of lightactivation of ATP hydrolysis (Slooten, L. and Nuyten, A., (1981) Biochim. Biophys. Acta 638, 305–312) are discussed.     

Intergeneric structural variability of the primary donor of photosynthetic bacteria: Resonance raman spectroscopy of reaction centers from two Rhodospirillum and Rhodobacter species

Several structural properties of the primary donor of Rhodobacter sphaeroides, wild type, have been obtained recently from difference resonance Raman spectra (Robert, B. and Lutz, M. (1986) Biochemistry 5, 2303–2309). In order to test the interspecific variability of the primary donor structure, we extended those observations to reaction centers of Rhodospirillum rubrum, wild type, using the same difference methods. Difference resonance Raman spectra of the primary donor are extremely close to those obtained for Rhb. sphaeroides. Identical conclusions can be drawn for the two species about the molecular interaction states of the magnesium atoms and of the acetyl carbonyl groups of both bacteriochlorophyll a molecules constituting their primary donors. However, the keto carbonyl of one of the bacteriochlorophylls, which is intermolecularly bound in Rhb. sphaeroides, is free from bonding in Rsp. rubrum. It thus appears that there is a limited interspecific variability of the structure of the primary donor in Rhodospirillales. These results also demonstrate an interspecifically variable, environmental asymmetry around the two primary donor molecules, which should variably affect charge distributions over these two molecules, in transient intermediates states of P, according to the species considered.     

Delayed fluorescence from Rhodopseudomonas sphaeroides reaction centers. Enthalpy and free energy changes accompanying electron transfer from P-870 to quinones

Delayed fluorescence from isolated reaction centers of Rhodopseudomonas sphaeroides was measured to study the energetics of electron transfer from the bacteriochlorophyll complex (P-870, or P) to the primary and secondary quinones (Q_A and Q_B). The analysis was based on the assumption that electron transfer between P and Q reaches equilibrium quickly after flash excitation, and stays in equilibrium during the lifetime of the P⁺Q⁻ radical pair. Delayed fluorescence of 1Q reaction centers (reaction centers that contain only Q_A) has a lifetime of about 0.1 s, which corresponds to the decay of P⁺Q⁻_A. 2Q reaction centers (which contain both Q_A and Q_B) have a much weaker delayed fluorescence, with a lifetime that corresponds to that of P⁺Q⁻_B (about 1 s). In the presence of o-phenanthroline, the delayed fluorescence of 2Q reaction centers becomes similar in intensity and decay kinetics to that of 1Q reaction centers. From comparisons of the intensities of the delayed fluorescence from P⁺Q⁻_A and P⁺Q⁻_B, the standard free energy difference between P⁺Q⁻_A and P⁺Q⁻_B is calculated to be 78 ± 8 meV. From a comparison of the intensity of the delayed fluorescence with that of prompt fluorescence, we calculate that P⁺Q⁻_A is 0.86 ± 0.02 eV below the excited singlet state of P in free energy, or about 0.52 eV above the ground state PQ_A. The temperature dependence of the delayed fluorescence indicates that P⁺Q⁻_A is about 0.75 eV below the excited singlet state in enthalpy, or about 0.63 eV above the ground state.     

Photosynthetic unit size and electron-transport chain in a photoreaction center-depleted mutant of Rhodospirillum rubrum

The aim of this work was to explain the relatively fast growth of a mutant of Rhodospirillum rubrum (F24.1) which contains 7–8% of an apparently normal photoreaction center. We explored the double hypothesis that the size of its photosynthetic unit is larger than that of the wild type and that its electron-transport chain is organized in a network rather than in isolated loops. The first feature would allow faster growth under less than saturating light intensities and the second would allow faster maximal electron fluxes than would be predicted from the photoreaction center content. With respect to the first possibility, measurements of absorbance changes at 793 nm induced by short flashes of increasing intensity indicate that the photosynthetic unit of strain F24.1 is 5.6-fold larger than that of strain S1. The second possibility was verified by measuring relative electron fluxes at the photoreaction center in the two strains. This was established in the steady state from the amount of primary donor oxidized by a continuous light beam of increasing intensity. This electron flux was found to be about 70% as high in strain F24.1 as in strain S1. A more detailed study of the electron-transport chain indicated that cytochrome c₂ is by far the main secondary electron donor in strain F24.1. No evidence could be obtained for the existence of another secondary donor in that strain. The mole ratio of cytochrome c₂ to photoreaction center is about 6 in strain F24.1 as conpared to about 0.5 in strain S1. In strain 24.1, the pool of secondary donor appears to be collectively involved in the reduction of the oxidized primary donor. The replacement time at the photoreaction center of a first equivalent of oxidized cytochrome c₂ by a second equivalent of reduced cytochrome c₂ is less than or equal to 0.2 ms. The effect of the photoreaction center content on the size of the photosynthetic unit is discussed in terms of the different models proposed for the organisation of the photosynthetic unit. We propose that the electron-transport chain is organized in a network, perhaps by virtue of the lateral mobility of some of the electron carriers such as ubiquinone and cytochrome c₂.     

Model studies of low-temperature optical transitions of photosynthetic reaction centers A-, LD-, CD-, ADMR- and LD-ADMR-spectra for Rhodopseudomonas viridis

The optical spectra of the reaction center (RC) of Rhodopseudomonas viridis including absorption (A), linear dichrosism (LD), circular dichroism (CD), absorption-detected magnetic resonance (ADMR) and its linear dichroism (LD-ADMR) are simulated by an exciton model. It involves the Q_y transitions of six prosthetic groups: four (bacteriochlorophyll-b molecules, two bacteriopheophytin-b molecules and the Soret bands B_y of the special-pair pigments, which couple most strongly with the corresponding Q_y transitions. For the ADMR-spectra additional excitations of the special-pair triplet are introduced. While interactions between the Q_y transitions and the B_y transitions are in principle determined from the structural arrangement of the pigments, the interactions to the other states are adjusted to fit the spectral features for the various transitions. The interaction of the newly introduced states are interpreted in terms of a simple model.     

Properties of the reaction center of the thermophilic purple photosynthetic bacterium Chromatium tepidum

Reaction centers were purified from the thermophilic purple sulfur photosynthetic bacterium Chromatium tepidum. The reaction center consists of four polypeptides L, M, H and C, whose apparent molecular masses were determined to be 25, 30, 34 and 44 kDa, respectively, by polyacrylamide gel electrophoresis. The heaviest peptide corresponds to tightly bound cytochrome. The tightly bound cytochrome c contains two types of heme, high-potential c-556 and low-potential c-553. The low-potential heme is able to be photooxidized at 77 K. The reaction center exhibits laser-flash-induced absorption changes and circular dichroism spectra similar to those observed in other purple photosynthetic bacteria. Whole cells contain both ubiquinone and menaquinone. Reaction centers contain only a single active quinone; chemical analysis showed this to be menaquinone. Reaction center complexes without the tightly bound cytochrome were also prepared. The near-infrared pigment absorption bands are red-shifted in reaction centers with cytochrome compared to those without cytochrome.     

Probing the topology of proteins in the chromatophore membrane of Rhodospirillum rubrum G-9 with proteinase K

All the major membrane proteins of isolated chromatophore vesicles are eventually degraded upon incubation with the unspecific proteinase K. These proteins must therefore be exposed at least partially or temporarily on the cytosolic surface of the membrane which is exclusively accessible to the proteinase in intact chromatophore vesicles. That the vesicles are intact during the incubation with proteinase is demonstrated by the finding that cytochrome c₂, which is located in the interior of the vesicles, is protected from proteolytic attack. The degree of degradation of the various chromatophore proteins and the time taken for degradation differ characteristically. From the changes in intensity of the gel bands during the course of digestion it appears that reaction center subunit H is digested first, much faster than are subunits M and L. The near-infrared absorption spectrum of the chromatophores changes only after proteolytic degradation of these two pigment-carrying subunits. Fading of the band of the light-harvesting polypeptide is evident only after prolonged incubation. It seems that this is the most stable component of the chromatophore membrane. The light-harvesting polypeptide appears to be somewhat shortened eventually, leaving the protein conformation necessary for holding the pigments unchanged, as shown by the absorption spectrum. The possible topology of these major membrane components is discussed in the light of these findings.     

Rotational mobility of the photoreaction center in chromatophore membranes of Rhodospirillum rubrum

We investigated the rotational mobility of the photoreaction center in chromatophores of Rhodospirillum rubrum by studying the photoinduced linear dichroism of absorption changes at 865 nm. The study was carried out in suspensions of chromatophores treated with ferricyanide in order to bleach their antenna bacteriochlorophyll and thus minimize depolarization by energy transfer. Very little depolarization of the photoinduced absorbance change at 865 nm was observed at room temperature for chromatophores immersed in a highly viscous medium over the time range 0–10 ms following an exciting light flash. In the light of independent evidence for transmembrane arrangement of the photoreaction center, we conclude that the photoreaction center protein is immobilized in the chromatophore membrane for at least 10 ms.     

Comparative and evolutionary aspects of the photosynthetic electron transfer system of purple bacteria

The cyclic electron transfer system in purple bacteria is composed of the photosynthetic reaction center, the cytochromebc ₁ complex, cytochromec ₂, and ubiquinone. These components share many characteristics with those of photosynthesis and respiration in other organisms. Studies of the cyclic electron transfer system have provided useful insights about the evolution and general mechanisms of membranous energy-conserving systems. The photosynthetic system in purple bacteria may represent a prototype of highly efficient, energy-conserving electron transfer systems in the organisms. Recipient of the Botanical Society Award of Young Scientists, 1992     

On the mechanism of photosynthetic electron transfer in Rhodopseudomonas capsulata and Rhodopseudomonas sphaeroides

(1) Current models for the mechanism of cyclic electron transport in Rhodopseudomonas sphaeroides and Rhodopseudomonas capsulata have been investigated by observing the kinetics of electron transport in the presence of inhibitors, or in photosynthetically incompetent mutant strains. (2) In addition to its well-characterized effect on the Rieske-type iron sulfur center, 5-(n-undecyl)-6-hydroxy-4,7-dioxobenzothiazole (UHDBT) inhibits both cytochrome b₅₀ and cytochrome b_?90 reduction induced by flash excitation in Rps. sphaeroides and Rps. capsulata. The concentration dependency of the inhibition in the presence of antimycin (approx. 2.7 mol UHDBT/mol reaction center for 50% inhibition of extent) is very similar to that of its inhibition of the antimycin-insensitive phase of ferricytochrome c re-reduction. UHDBT did not inhibit electron transfer between the reduced primary acceptor ubiquinone (Q^?_I) and the secondary acceptor ubiquinone (Q_II) of the reaction center acceptor complex. A mutant of Rps. capsulata, strain R126, lacked both the UHDBT and antimycin-sensitive phases of cytochrome c re-reduction, and ferricytochrome b₅₀ reduction on flash excitation. (3) In the presence of antimycin, the initial rate of cytochrome b₅₀ reduction increased about 10-fold as the E_h(7.0) was lowered below 180 mV. A plot of the rate at the fastest point in each trace against redox potential resembles the Nernst plot for a two-electron carrier with E_m(7.0) ≈ 125 ± 15 mV. Following flash excitation there was a lag of 100–500 μs before cytochrome b₅₀ reduction began. However, there was a considerably longer lag before significant reduction of cytochrome c by the antimycin-sensitive pathway occurred. (4) The herbicide ametryne inhibited electron transfer between Q^?_I and Q_II. It was an effective inhibitor of cytochrome b₅₀ photoreduction at E_h(7.0) 390 mV, but not at E_h(7.0) 100 mV. At the latter E_h, low concentrations of ametryne inhibited turnover after one flash in only half of the photochemical reaction centers. By analogy with the response to o-phenanthroline, it is suggested that ametryne is ineffective at inhibiting electron transfer from Q^?_I to the secondary acceptor ubiquinone when the latter is reduced to the semiquinone form before excitation. (5) At E_h(7.0) > 200 mV, antimycin had a marked effect on the cytochrome b₅₀ reduction-oxidation kinetics but not on the cytochrome c and reaction center changes or the slow phase III of the electrochromic carotenoid change on a 10-ms time scale. This observation appears to rule out a mechanism in which cytochrome b₅₀ oxidation is obligatorily and kinetically linked to the antimycin-sensitive phase of cytochrome c reduction in a reaction involving transmembrane charge transfer at high E_h values. However, at lower redox potentials, cytochrome b₅₀ oxidation is more rapid, and may be linked to the antimycin-sensitive reduction of cytochrome c. (6) It is concluded that neither a simple linear scheme nor a simple Q-cycle model can account adequately for all the observations. Future models will have to take account of a possible heterogeneity of redox chains resulting from the two-electron gate at the level of the secondary quinone, and of the involvement of cytochrome b_?90 in the rapid reactions of the cyclic electron transfer chain     

Magnetic field-stimulated luminescence and a matrix model for energy transfer. A new method for determining the redox state of the first quinone acceptor in the reaction center of whole cells of Rhodospirillum rubrum

In whole cells of Rhodospirillum rubrum the light-induced absorbance difference spectrum of the reduction of the first quinone electron acceptor Q₁ was determined in order to relate the emission yield ф and the magnetic field-induced emission increase Δф to the redox state of Q₁. It was found that Δф/ф² is a linear function of the number of reaction centers, in which Q₁ is reduced, independent of the fraction of reaction centers in the oxidized state. The emission yield is a hyperbolic function of the fraction of reaction centers closed, either by reduction of the acceptor Q₁ or by oxidation of the primary electron donor P. Apparently, in whole cells of R. rubrum a matrix model for energy transfer between various photosynthetic units can be applied. A model is presented, which is a generalization of theoretical considerations reported before (Duysens, L.N.M. (1978) in Chlorophyll Organization and Energy Transfer in Photosynthesis, Ciba Found. Symp. 61 (New Series), pp. 323–340, Elsevier/North-Holland, Amsterdam) and which is in excellent agreement with the experiments. From simultaneous measurements of Δф and ф the redox state of the reaction center can relatively easily be determined. So far, this is the only method for simultaneously measuring the fractions P⁺ and Q⁻₁ in intact cells under steady-state conditions.     

Resolved difference spectra of redox centers involved in photosynthetic electron flow in Rhodopseudomonas capsulata and rhodopseudomonas sphaeroides

1. In Rhodopseudomonas sphaeroides the Q_x absorption band of the reaction center bacteriochlorophyll dimer which bleaches on photo-oxidation is both blue-shifted and has an increased extinction coefficient on solubilisation of the chromatophore membrane with lauryldimethylamine-N-oxide. These effects may be attributable in part to the particle flattening effect.2. The difference spectrum of photo-oxidisable c type cytochrome in the chromatophore was found to have a slightly variable peak position in the α-band (λ_max at 551–551.25 nm); this position was always red-shifted in comparison to that of isolated cytochrome c₂ (λ_max at 549.5 ± 0.5 nm). The shift in wavelength maximum was not due to association with the reaction center protein. A possible heterogeneity in the c-type cytochromes of chromatophores is discussed.3. Flash-induced difference spectra attributed to cytochrome b were resolved at several different redox potentials and in the presence and absence of antimycin. Under most conditions, one major component, cytochrome b₅₀ appeared to be involved. However, in some circumstances, reduction of a component with the spectral characteristics of cytochrome b_?90 was observed.4. Difference spectra attributed to (BChl)₂, Q^?_II, c type cytochrome and cytochrome b₅₀ were resolved in the Soret region for Rhodopseudomonas capsulata.5. A computer-linked kinetic spectrophotometer for obtaining automatically the difference spectra of components functioning in photosynthetic electron transfer chains is described. The system incorporates a novel method for automatically adjusting and holding the photomultiplier supply voltage.     

Labeling of chromatophore membranes and reaction centers from the photosynthetic bacterium Rhodospirillum rubrum with the hydrophobic marker 5-[125I]iodonaphthyl-1-azide

Chromatophores of the photosynthetic bacterium Rhodospirillum rubrum and isolated reaction centers were labeled with the lipophilic membrane marker 5-[¹²⁵I]iodonaphthyl-1-azide. The two smaller reaction center proteins L and M bind more label than the larger subunit H, a fact supporting the proposed localisation of the 3 subunits obtained with hydrophilic labels. Besides these integral proteins the lipids, among them mainly the pigments and the quinones, are highly labeled suggesting a hydrophobic environment around these molecules and a preferred reactivity to iodonaphthylazide. Such a hydrophobic environment may be of great importance for the function of the photosynthetic reaction centers especially for the charge separation and the primary reactions in electron transport.