Trapping, loss and annihilation of excitations in a photosynthetic system: II. Experiments with the purple bacteria Rhodospirillum rubrum and Rhodopseudomonas capsulata

In this paper a number of experiments with the purple bacteria Rhodospirillum rubrum and Rhodopseudomonas capsulata is described in which the total fluorescence yield and/or the total fraction of reaction centers closed after a picosecond laser pulse were measured as a function of the pulse intensity. The conditions were such that the reaction centers were either all in the open or all in the closed state before the pulse arrived. These experiments are analysed using the theoretical formalism discussed in the preceding paper (Den Hollander, W.T.F., Bakker J.G.C., and Van Grondelle, R., Biochim. Biophys. Acta 725, 492–507). From the experimental results the number of connected photosynthetic units, λ, the rate of energy transfer between neighboring antenna molecules, k_h, and the rate of trapping by an open reaction center, k^o_t, can be estimated. For R. rubrum it is found that λ = 14−17, k_h = (1−2)·10¹² s⁻¹ and k^o_t = (4−6)·10¹¹ s⁻¹, for Rps. capsulata λ ≈ 30, k_h ≈ 4·10¹¹ s⁻¹ and k^o_t ≈ 3·10¹¹ s⁻¹. The findings are discussed in terms of current models for the structure of the antenna and the kinetic properties of the decay processes occurring in these purple bacteria.     

Carotenoid triplet states in reaction centers from Rhodopseudomonas sphaeroides and Rhodospirillum rubrum

Purified photochemical reaction centers from three strains of Rhodopseudomonas sphaeroides and two of Rhodospirillum rubrum were reduced with Na₂S₂O₄ so as to block their photochemical electron transfer reactions. They then were excited with flashes lasting 5–30 ns. In all cases, absorbance measurements showed that the flash caused the immediate formation of a transient state (P^F) which had been detected previously in reaction centers from Rps. sphaeroides strain R26. Previous work has shown that state P^F is an intermediate in the photochemical electron transfer reaction in the reaction centers of that particular strain, and the present work generalizes that conclusion.

In the reaction centers from two strains that lack carotenoids (Rps. sphaeroides R26 and R. rubrum G9), the decay of P^F yields a longer-lived state (P^R) which is probably a triplet state of the bacteriochlorophyll of the reaction center. In the R26 preparation, the decay of P^F was found to have a half-time of 10±2 ns. The decay kinetics rule out the identification of P^F as the fluorescent excited singlet state of the reaction center.

In the reaction centers from three strains that contain carotenoids (Rps sphaeroides 2.4.1 and Ga, and R. rubrum S1), state P^R was not detected, and the decay of P^F generated triplet states of carotenoids. The efficiency of the coupling between the decay of P^F and the formation of the carotenoid triplet appeared to be close to 100% at room temperature, but somewhat lower at 77 °K. Taken with previous results, this suggests that the coupling is direct and does not require the intermediate formation of state P^R. This conclusion would be consistent with the view that P^F is a biradical which can be triplet in character.     

Fluorescence of bacteriochlorophyll as related to the photochemistry of chromatophores of photosynthetic bacteria

Time courses and the emission spectra of fluorescence and light-induced absorption changes of P890 in chromatophores of the photosynthetic bacteria Chromatium D, Rhodopseudomonas spheroides and Rhodospirillum rubrum were investigated.

The time course of fluorescence in chromatophores was separated into two phases, i.e. an initial rapid rise (ƒ_i) and a subsequent slow increase towards a steady level of emission (ƒ_v). The ƒ_i and the ƒ_v components showed different emission spectra having different peak position. The ƒ_v component was emitted from the longest wavelength-absorbing form of bulk bacteriochlorophyll (B890), the ƒ_i component from both B890 and B850.

The magnitude of the ƒ_v component depended on experimental conditions controlling the states of the cyclic electron transport in chromatophores, including changes in levels of redox potential of the medium, additions of electron donors and inhibitors. The magnitude of the ƒ_i component was not affected by these experimental conditions. It was, therefore, concluded that only the ƒ_v component is related to the cyclic electron transport, and that the magnitude of ƒ_v is controlled by the oxidation-reduction state of the primary electron acceptor for the photochemical reaction center in chromatophores.     

Fluorescence characteristics of lyophilized maize chloroplasts suspended in buffer

Fluorescence transients were measured in lyophilized maize chloroplasts (suspended in Tris-maleate buffer (pH 6.6)) after extraction with heptane. (The fluorescence characteristics before extraction were qualitatively similar to those in the fresh chloroplasts.) The initial fluorescence level (m) in the (dry) heptane-extracted sample remained the same as in the unextracted material, but the variable fluorescence (Δm) was drastically diminished. A portion of variable fluorescence, however, could be restored by adding Na₂S₂O₄. If the heptane extraction was made in the presence of water (wet), the m level was almost as high as (or higher than) the final level (M) of the unextracted sample, and Δm was reduced. The “jet” of O₂ (that measures the pool size of the intersystem intermediate A) and the “microjet” (that measures the pool size of the reaction center complex E), present in the unextracted samples, were absent in both types of extracted samples. Some of the above data may be interpreted in a hypothesis in which two quenchers (Q₁ and Q₂) control the fluorescence (O → P) of chloroplasts — the reduction of Q₁ being responsible for the rapid and that of Q₂ for the slow fluorescence rise.     

Limiting steps in Photosystem II and water decomposition in Chlorella and spinach chloroplasts

1. 1. By varying the redox potential of a chloroplast suspension, we obtained new evidence for an equilibrium between states S₀ and S₁ in the model of Kok, B., Forbush, B. and McGloin, N. (1970, Photochem. Photobiol. 11, 457–475). The mid-point potential of the S₀ to S₁ couple is close to that for the pool of the electron acceptor of System II, A to A⁻.

2. 2. The limiting steps between two consecutive photoreactions of System II in Chlorella and spinach chloroplasts, have been studied.

2.1. (a) The limiting step from S₁ to S₂ (noted γ₁ (Δt)) is not exponential. Its temperature coefficient becomes greater as the reaction proceeds. The shape of the kinetics is an intrinsic property of each center. Chloroplasts fixed with 2% glutaraldehyde, show simple first order kinetics.

2.2. (b) The limiting step from S₀ to S₁ (γ₀ (Δt)) exhibits the same characteristics as γ₁ (Δt)).

2.3. (c) The limiting step from S₂ to S₃ (γ₂ (Δt)) shows sigmoidal kinetics; two reactions are involved. One of the reactions exhibits the same properties as γ₀ (Δt) and γ₁ (Δt).

2.4. (d) The limiting step from S₃ to S₀ (γ₃ (Δt)) is a first order reaction, two times slower than the other transitions. This reaction is interpretated in terms of oxygen release.

3. 3. We also studied the limiting steps in the presence of low concentrations (50 μM) of hydroxylamine. The results favor the binding of two molecules of hydroxylamine to every photochemical center.

Phenotypic analysis of the ccp1Delta and ccp1Delta-ccp1W191F mutant strains of Saccharomyces cerevisiae indicates that cytochrome c peroxidase functions in oxidative-stress signaling

Yeast cytochrome c peroxidase (CCP) efficiently catalyzes the reduction of H₂O₂ to H₂O by ferrocytochrome c in vitro. The physiological function of CCP, a heme peroxidase that is targeted to the mitochondrial intermembrane space of Saccharomyces cerevisiae, is not known. CCP1-null-mutant cells in the W303-1B genetic background (ccp1Δ) grew as well as wild-type cells with glucose, ethanol, glycerol or lactate as carbon sources but with a shorter initial doubling time. Monitoring growth over 10 days demonstrated that CCP1 does not enhance mitochondrial function in unstressed cells. No role for CCP1 was apparent in cells exposed to heat stress under aerobic or anaerobic conditions. However, the detoxification function of CCP protected respiring mitochondria when cells were challenged with H₂O₂. Transformation of ccp1Δ with ccp1^W191F, which encodes the CCP^W191F mutant enzyme lacking CCP activity, significantly increased the sensitivity to H₂O₂ of exponential-phase fermenting cells. In contrast, stationary-phase (7-day) ccp1Δ-ccp1^W191F exhibited wild-type tolerance to H₂O₂, which exceeded that of ccp1Δ. Challenge with H₂O₂ caused increased CCP, superoxide dismutase and catalase antioxidant enzyme activities (but not glutathione reductase activity) in exponentially growing cells and decreased antioxidant activities in stationary-phase cells. Although unstressed stationary-phase ccp1Δ exhibited the highest catalase and glutathione reductase activities, a greater loss of these antioxidant activities was observed on H₂O₂ exposure in ccp1Δ than in ccp1Δ-ccp1^W191F and wild-type cells. The phenotypic differences reported here between the ccp1Δ and ccp1Δ-ccp1^W191F strains lacking CCP activity provide strong evidence that CCP has separate antioxidant and signaling functions in yeast.     

Probing fluorescence induction in chloroplasts on a nanosecond time scale utilizing picosecond laser pulse pairs

The fluorescence induction and other fluorescence properties of spinach chloroplasts at room temperature were probed utilizing two 30-ps wide laser pulses (530 nm) spaced Δt (s) apart in time (Δt = 5–110 ns). The energy of the first pulse (P₁) was varied (10¹²–10¹⁶ photons · cm⁻²), while the energy of the second (probe) pulse (P₂) was held constant (5 · 10¹³ photons · cm⁻²). A gated (10 ns) optical multichannel analyzer-spectrograph system allowed for the detection of the fluorescence generated either by P₁ alone, or by P₂ alone (preceded by P₁). The dominant effect observed for the fluorescence yield generated by P₁ alone is the usual singlet-singlet exciton annihilation which gives rise to a decrease in the yield at high energies. However, when the fluorescence yield of dark-adapted chloroplasts is measured utilizing P₂ (preceded by pulse P₁) an increase in this yield is observed. The magnitude of this increase depends on Δt, and is characterized by a time constant of 28 ± 4 ns. This rise in the fluorescence yield is attributed to a reduction of the oxidized (by P₁) reaction center P-680⁺ by a primary donor. At high pulse energies (P₁ = 4 · 10¹⁴ photons · cm⁻²) the magnitude of this fluorescence induction is diminished by another quenching effect which is attributed to triplet excited states generated by intense P₁ pulses. Assuming that the P₁ pulse energy dependence of the fluorescence yield rise reflects the closing of the reaction centers, it is estimated that about 3–4 photon hits per reaction center are required to close completely the reaction centers, and that there are 185–210 chlorophyll molecules per Photosystem II reaction center.     

Transfer of light-induced electron-spin polarization from the intermediary acceptor to the prereduced primary acceptor in the reaction center of photosynthetic bacteria

In reaction centers and chromatophores of photosynthetic bacteria strong light-induced emissive ESR signals have been found, not only after a flash, but also under continuous illumination. The signal, with g = 2.0048 and ΔH_pp = 7.6 G, is only present under reducing conditions in material in which the primary acceptor, ubiquinone, U and its associated high-spin ferrous ion are magnetically uncoupled. Its amplitude under continuous illumination is strongly dependent on light intensity and on microwave power.

The emissive signal is attributed to the prereduced primary acceptor, U⁻, which becomes polarized through transfer of spin polarization by a magnetic exchange interaction with the photoreduced, spin polarized intermediary acceptor, I⁻. A kinetic model is presented which explains the observed dependence of emissivity on light intensity and microwave power. Applying this analysis to the light saturation data, a value of the exchange rate between I⁻ and U⁻ of 4 · 10⁸ s⁻¹ is derived, corresponding to an exchange interaction of 3–5 G.     

Photosystem I photochemistry at low temperature. Heterogeneity in pathways for electron transfer to the secondary acceptors and for recombination processes

Electron transport has been studied by flash absorption and EPR spectroscopies at 10–30 K in Photosystem I particles prepared with digitonin under different redox conditions. In the presence of ascorbate, an irreversible charge separation is progressively induced at 10 K between P-700 and iron-sulfur center A by successive laser flashes, up to a maximum which corresponds to about two-thirds of the reaction centers. In these centers, heterogeneity of the rate for center A reduction is also shown. In the other third of reaction centers, the charge separation is reversible and relaxes with a t_1/2 ≈ 120 μs. When the iron-sulfur centers A and B are prereduced, the 120 μs relaxation becomes the dominant process (70–80% of the reaction centers), while a slow component (t_1/2 = 50–400 ms) reflecting the recombination between P-700⁺ and center X⁻ occurs in a minority of reaction centers (10–15%). Flash absorption and EPR experiments show that the partner of P-700⁺ in the 120 μs recombination is neither X nor a chlorophyll but more probably the acceptor A⁻₁ as defined by Bonnerjea and Evans (Bonnerjea, J. and Evans, M.C.W. (1982) FEBS Lett. 148, 313–316). The role of center X in low-temperature electron flow is also discussed.     

Evidence for slow turnover in a fraction of Photosystem II complexes in thylakoid membranes

We used two different techniques to measure the recovery time of Photosystem II following the transfer of a single electron from P-680 to Q_A in thylakoid membranes isolated from spinach. Electron transfer in Photosystem II reaction centers was probed first by spectroscopic measurements of the electrochromic shift at 518 nm due to charge separation within the reaction centers. Using two short actinic flashes separated by a variable time interval we determined the time required after the first flash for the electrochromic shift at 518 nm to recover to the full extent on the second flash. In the second technique the redox state of Q_A at variable times after a saturating flash was monitored by measurement of the fluorescence induction in the absence of an inhibitor and in the presence of ferricyanide. The objective was to determine the time required after the actinic flash for the fluorescence induction to recover to the value observed after a 60 s dark period. Measurements were done under conditions in which (1) the electron donor for Photosystem II was water and the acceptor was the endogenous plastoquinone pool, and (2) Q₄₀₀, the Fe²⁺ near Q_A, remained reduced and therefore was not a participant in the flash-induced electron-transfer reactions. The electrochromic shift at 518 nm and the fluorescence induction revealed a prominent biphasic recovery time for Photosystem II reaction centers. The majority of the Photosystem II reaction centers recovered in less than 50 ms. However, approx. one-third of the Photosystem II reaction centers required a half-time of 2–3 s to recover. Our interpretation of these data is that Photosystem II reaction centers consist of at least two distinct populations. One population, typically 68% of the total amount of Photosystem II as determined by the electrochromic shift, has a steady-state turnover rate for the electron-transfer reaction from water to the plastoquinone pool of approx. 250 e⁻ / s, sufficiently rapid to account for measured rates of steady-state electron transport. The other population, typically 32%, has a turnover rate of approx. 0.2 e⁻ / s. Since this turnover rate is over 1000-times slower than normally active Photosystem II complexes, we conclude that the slowly turning over Photosystem II complexes are inconsequential in contributing to energy transduction. The slowly turning over Photosystem II complexes are able to transfer an electron from P-680 to Q_A rapidly, but the reoxidation of Q⁻_A is slow (t1/2 = 2 s). The fluorescence induction measurements lead us to conclude that there is significant overlap between the slowly turning over fraction of Photosystem II complexes and PS II_β reaction centers. One corollary of this conclusion is that electron transfer from P-680 to Q_A in PS II_β reaction centers results in charge separation across the membrane and gives rise to an electrochromic shift.     

Mus81 functions in the quality control of replication forks at the rDNA and is involved in the maintenance of rDNA repeat number in Saccharomyces cerevisiae

Previous studies in yeast have suggested that the SGS1 DNA helicase or the Mus81-Mms4 structure-specific endonuclease is required to suppress the accumulation of lethal recombination intermediates during DNA replication. However, the structure of these intermediates and their mechanism of the suppression are unknown. To examine this reaction, we have isolated and characterized a temperature-sensitive (ts) allele of MUS81. At the non-permissive temperature, sgs1Δ mus81^ts cells arrest at G₂/M phase after going through S-phase. Bulk DNA replication appears complete but is defective since the Rad53 checkpoint kinase is strongly phosphorylated under these conditions. In addition, the induction of Rad53 hyper-phosphorylation by MMS was deficient at permissive temperature. Analysis of rDNA replication intermediates at the non-permissive temperature revealed elevated pausing of replication forks at the RFB in the sgs1Δ mus81^ts mutant and a novel linear structure that was dependent on RAD52. Pulsed-field gel electrophoresis of the mus81Δ mutant revealed an expansion of the rDNA locus depending on RAD52, in addition to fragmentation of Chr XII in the sgs1Δ mus81^ts mutant at permissive temperature. This is the first evidence that Mus81 functions in quality control of replication forks and that it is involved in the maintenance of rDNA repeats in vivo.     

Kinetics and mechanism of the stoichiometric oxygenation of [Cu(fla)(idpa)]ClO4 [fla=flavonolate, IDPA=3,3′-imino-bis(N,N-dimethylpropylamine)] and the [Cu(fla)(idpa)]ClO4-catalysed oxygenation of flavonol

Oxygenation of [Cu^II(fla)(idpa)]ClO₄ (fla=flavonolate; IDPA=3,3′-iminobis(N,N-dimethylpropylamine)) in dimethylformamide gives [Cu^II(idpa)(O-bs)]ClO₄ (O-bs=O-benzoylsalicylate) and CO. The oxygenolysis of [Cu^II(fla)(idpa)]ClO₄ in DMF was followed by electronic spectroscopy and the rate law −d[{Cu^II(fla)(idpa)}ClO₄]/dt=k_obs[{Cu^II(fla)(idpa)}ClO₄][O₂] was obtained. The rate constant, activation enthalpy and entropy at 373 K are k_obs=6.13±0.16×10⁻³ M⁻¹ s⁻¹, ΔH^‡=64±5 kJ mol⁻¹, ΔS^‡=−120±13 J mol⁻¹ K⁻¹, respectively. The reaction fits a Hammett linear free energy relationship and a higher electron density on copper gives faster oxygenation rates. The complex [Cu^II(fla)(idpa)]ClO₄ has also been found to be a selective catalyst for the oxygenation of flavonol to the corresponding O-benzoylsalicylic acid and CO. The kinetics of the oxygenolysis in DMF was followed by electronic spectroscopy and the following rate law was obtained: −d[flaH]/dt=k_obs[{Cu^II(fla)(idpa)}ClO₄][O₂]. The rate constant, activation enthalpy and entropy at 403 K are k_obs=4.22±0.15×10⁻² M⁻¹ s⁻¹, ΔH^‡=71±6 kJ mol⁻¹, ΔS^‡=−97±15 J mol⁻¹ K⁻¹, respectively.     

Flavonoid Deactivation of Ferrylmyoglobin in Relation to Ease of Oxidation as Determined by Cyclic Voltammetry

Fourteen flavonoid aglycones, and the flavonoid glyco-side rutin, with redox potentials ranging from 0.20 (myricetin) to 0.83 V (chrysin) vs. NHE, as determined by cyclic voltammetry at 23°C in aqueous 50 mM phosphate, ionic strength 0.16 (NaCI) with pH = 7.4 and compared with redox potentials determined for four cinnamic acid derivatives, were all found to reduce ferrylmyoglobin, MbFe(IV)=O, to metmyoglo-bin, MbFe(III). Reaction stoichiometry depends strongly on the number of hydroxyl groups in the flavonoid B-ring. All compounds with 3',4'-dihydroxy substitution reduce 2 equivalents of MbFe(IV)=O, whereas naringenin, hesperitin and kaempferol, with one hydroxyl group in the B-ring, reduce with a one-to-one stoichiometry. As studied spectrophotometrically under pseudo-first-order conditions with flavonoids in excess, rutin and apigenin react with MbFe(IV)=O with very similar and moderately high activation enthalpies of ΔH‡₂₉₈ = 69 ± 1kJ mol^-1 and ΔH‡₂₉₈ = 65 ± 3kJ mol-¹, respectively, and with positive activation entropies of ΔH‡₂₉₈ = 23 ± 4Jmol-¹ K^-1 and ΔS‡₂₉₈ = 13 ± 9Jmol^-1K-¹, respectively, in agreement with outer-sphere electron transfer as rate determining. For the fifteen plant polyphenols only qualitative relations exist between redox potential and rate constants rather than a linear free energy relationship (r² = 0.503), and especially the flavone apigenin was found more efficient as reducing agent. For the flava-nones, a linear relation (r² = 0.971) indicate that, in the absence of a 2,3 double bond, removal of the 4-carbonyl group or addition of a 3-hydroxy group only has minor effect on reactivity. The flavonols are the most efficient reducing agents, effectively reducing MbFe(IV)=O to MbFe(III) and establishing a steady state distribution between the flavonol and MbFe(III) and oxymyoglobin, MbFe(II)O₂. Oxidised flavonols reduces MbFe(III) to MbFe(II)0₂ very efficiently and much faster than the parent flavonol.     

The sodium cycle. II. Na-coupled oxidative phosphorylation in Vibrio alginolyticus cells

The role of Na⁺ in Vibrio alginolyticus oxidative phosphorylation has been studied. It has been found that the addition of a respiratory substrate, lactate, to bacterial cells exhausted in endogenous pools of substrates and ATP has a strong stimulating effect on oxygen consumption and ATP synthesis. Phosphorylation is found to be sensitive to anaerobiosis as well as to HQNO, an agent inhibiting the Na⁺-motive respiratory chain of V. alginolyticus. Na⁺ loaded cells incubated in a K⁺ or Li⁺ medium fail to synthesize ATP in response to lactate addition. The addition of Na⁺ at a concentration comparable to that inside the cell is shown to abolish the inhibiting effect of the high intracellular Na⁺ level. Neither lactate oxidation nor Δω generation coupled with this oxidation is increased by external Na⁺ in the Na⁺-loaded cells. It is concluded that oxidative ATP synthesis in V. alginolyticus cells is inhibited by the artificially imposed reverse ΔPNa, i.e., [Na⁺]_in > [Na⁺]_out. Oxidative phosphorylation is resistant to a protonophorous uncoupler (0.1 mM CCCP) in the K⁺-loaded cells incubated in a high Na⁺ medium, i.e., when ΔpNa of the proper direction ([Na⁺]_in < [Na⁺]_out) is present. The addition of monensin in the presence of CCCP completely arrests the ATP synthesis. Monensin without CCCP is ineffective. Oxidative phosphorylation in the same cells incubated in a high K⁺ medium (ΔpNa is low) is decreased by CCCP even without monensin. Artificial formation of ΔpNa by adding 0.25 M NaCl to the K⁺-loaded cells (Na⁺ pulse) results in a temporary increase in the ATP level which spontaneously decreases again within a few minutes. Na⁺ pulse-induced ATP synthesis is completely abolished by monensin and is resistant to CCCP, valinomycin and HQNO. 0.05 M NaCl increases the ATP level only slightly. Thus, V. alginolyticus cells at alkaline pH represent the first example of an oxidative phosphorylation system which uses Na⁺ instead of H⁺ as the coupling ion.     

Determination of free energies in reaction centers of Rb. sphaeroides

Magnetic field-dependent recombination measurements together with magnetic field-dependent triplet lifetimes (Chidsey, E.D., Takiff, L., Goldstein, R.A. and Boxer, S.G. (1985) Proc. Natl. Acad. Sci USA 82, 6850–6854) yield a free energy change ΔG(P⁺H⁻ − ³P*) = 0.165 eV ±0.008 at 290 K. This does not depend on whether nuclear spin relaxation in the state ³P* is assumed to be fast or slow compared to the lifetime of this state. This value, being (almost) temperature independent, indicates ΔG(P⁺H⁻ − ³P*) ΔH(P⁺H⁻ − ³P*) and is consistent with ΔG(¹P* − P⁺H⁻) and ΔH(¹P* − ³P*) from previous delayed fluorescence and phosphorescence data, implying ΔG ΔH for all combinations of these states.     

Heats of reaction of HMo(CO)3(C5R5) (R = H, CH3) with diphenyldisulfide and of formation of the clusters [PhSMo(CO)x(C5H5)]2, X = 1,2. Thermodynamic study of molybdenum-sulfur bond strengths

The enthalpies of reaction of HMo(CO)₃C₅R₅ (R = H, CH₃) with diphenyldisulfide producing PhSMo(CO)₃C₅R₅ and PhSH have been measured in toluene and THF solution (R = H, ΔH= −8.5 ± 0.5 kcal mol⁻¹ (tol), −10.8 ± 0.7 kcal mol⁻¹ (THF); R = CH₃, ΔH = −11.3±0.3 kcal mol⁻¹ (tol), −13.2±0.7 kcal mol⁻¹ (THF)). These data are used to estimate the Mo---SPh bond strength to be on the order of 38–41 kcal mol⁻¹ for these complexes. The increased exothermicity of oxidative addition of disulfide in THF versus toluene is attributed to hydrogen bonding between thiophenol produced in the reaction and THF. This was confirmed by measurement of the heat of solution of thiophenol in toluene and THF. Differential scanning calorimetry as well as high temperature calorimetry have been performed on the dimerization and subsequent decarbonylation reactions of PhSMo(CO)₃Cp yielding [PhSMo(CO)₂Cp]₂ and [PhSMo(CO)Cp]₂. The enthalpies of reaction of PhSMo(CO)₃Cp and [PhSMo(CO)₂Cp]₂ with PPh₃, PPh₂Me and P(OMe)₃ have also been measured. The disproportionation reaction: 2[PhSMo(CO)₂Cp]₂ → 2PhSMo(CO)₃Cp + [PhSMP(CO)Cp]₂ is reported and its enthalpy has also been measured. These data allow determination of the enthalpy of formation of the metal-sulfur clusters [PhSMo(CO)_nC₅H₅]₂, N = 1,2.     

Pigment content and molar extinction coefficients of photochemical reaction centers from Rhodopseudomonas spheroides

Reaction center particles isolated from carotenoidless mutant Rhodopseudomonas spheroides were studied with the aim of determining the pigment composition and the molar extinction coefficients.

Two independent sets of measurements using a variety of methods show that a sample with A_{800 nm} = 1.00 contains 20.8 ± 0.8 μM tetrapyrrole and that the ratio of bacteriochlorophyll to bacteriopheophytin is 2:1.

Measurements were made of the absorption changes attending the oxidation of cytochrome c coupled to reduction of the photooxidized primary electron donor in reaction centers, using laser flash excitation. The ratio of the absorption change at 865 nm (due to the bleaching of P870) to that at 550 nm (oxidation of cytochrome) was found to be 5.77.

These results, combined with other data, yield a pigment composition of 4 bacteriochlorophyll and 2 bacteriopheophytin molecules in a reaction center. Based on this choice, extinction coefficients are determined for the 802- and 865-nm bands: _{802 nm} = 288 (± 14) mM⁻¹ · cm⁻¹ and _{865 nm} = 128 (± 6) mM⁻¹ · cm⁻¹. For reversible bleaching of the 865-nm band, Δ^{red - ox}_865nm = 112 (± 6) mM⁻¹ · cm⁻¹ (referred to the molarity of reaction centers). Earlier reported values of photochemical quantum efficiency are recomputed, and the revised values are shown to be compatible with those obtained from measurements of fluorescence transients.     

The stereoisomerism of bacterial, reaction-center-bound carotenoids revisited: An electronic absorption, resonance Raman and H-NMR study

In order to solve discrepancies between earlier assignments we have reinvestigated the stereoisomerism of the spheroidene molecule bound to reaction centers (RC) of Rhodobacter sphaeroides. A stable cis isomer could be extracted and purified from the reaction centres by working at very low ambient light. Resonance Raman spectroscopy showed that this cis isomer assumed the same configuration as that of the RC-bound molecule. Proton-NMR spectroscopy of the extracted isomer permitted to assign it the 15–15′ mono cis configuration. Comparisons between resonance Raman spectra of the native form and of the 15 cis extract showed that, in the reaction center, 15 cis spheroidene is in addition twisted into a non-planar conformation. Comparisons of extraction-induced changes in relative intensities of Raman bands of the 760–1060 cm⁻¹ regions, which largely correspond to out-of-plane modes, further indicated that the out-of-plane twist of RC-bound spheroidene should predominantly affect C₈–C₁₂ and/or C_8′–C_12′ regions of the molecule rather than the central region. Comparisons between difference electronic absorption spectra of RC-bound spheroidene and of RC-bound methoxyneurosporene showed that the out-of-plane twisting of both these native forms results in a drastic weakening of their ¹C ← ¹A electronic transitions, compared with those of the planar, 15 cis forms. Finally, it is proposed, on the basis of their resonance Raman spectra, that spirilloxanthin bound to RCs of Rhodospirillum rubrum as well as dihydroneurosporene or dihydrolycopene bound to RCs of Rhodopseudomonas viridis shares 15 cis configurations and out-of-plane twisting with carotenoids bound to RCs of various strains of Rb. sphaeroides.     

Intracellular mitochondrial membrane potential as an indicator of hepatocyte energy metabolism: Further evidence for thermodynamic control of metabolism

The lipophilic triphenylmethylphosphonium cation (TPMP⁺) has been employed to measure ΔΨ_m, the electrical potential across the inner membrane of the mitochondria of intact hepatocytes. The present studies have examined the validity of this technique in hepatocytes exposed to graded concentrations of inhibitors of mitochondrial energy transduction. Under these conditions, TPMP⁺ uptake allows a reliable measure of ΔΨ_m in intracellular mitochondria, provided that the ratio [TPMP⁺]_i/[TPMP⁺]_e is greater than 50:1 and that at the end of the incubation more than 80% of the hepatocytes exclude Trypan blue. Hepatocytes, staining with Trypan blue, incubated in the presence of Ca²⁺, do not concentrate TPMP⁺. The relationships between ΔΨ_m and two other indicators of cellular energy state, ΔG_Pc and E_h, or between ΔΨ_m and J₀, were examined in hepatocytes from fasted rats by titration with graded concentrations of inhibitors of mitochondrial energy transduction. Linear relationships were generally observed between ΔΨ_m and ΔG_Pc, E_h or J₀ over the ΔΨ_m range of 120−160 mV, except in the presence of carboxyatractyloside or oligomycin, where ΔΨ_m remained constant. Both the magnitude and the direction of the slope of the observed relationships depended upon the nature of the inhibitor. Hepatocytes from fasted rats synthesized glucose from lactate or fructose, and urea from ammonia, at rates which were generally linear functions of the magnitude of ΔΨ_m, except in the presence of oligomycin or carboxyatractyloside. Linear relationships were also observed between ΔΨ_m and the rate of formation of lactate in cells incubated with fructose and in hepatocytes from fed rats. The linear property of these force-flow relationships is taken as evidence for the operation of thermodynamic regulatory mechanisms within hepatocytes.     

A study of dark luminescence in Chlorella. Background luminescence, 3-(3,4-dichlorophenyl)-1,1-dimethylurea-triggered luminescence and hydrogen peroxide chemiluminescence

Dark luminescence, defined as the ability of completely relaxed (darkadapted) photosynthetic systems to emit light, has been studied in Chlorella. Three main effects have been demonstrated. 3-(3,4-Dichlorophenyl)-1,1-dimethylurea elicits a weak emission L_D of very long lifetime (several minutes); it is believed to result from a negative shift of redox potential of the secondary System II electron acceptor B producing in some centers a state Q⁻ (reduced primary acceptor), as postulated by Velthuys and Amesz ((1974) Biochim. Biophys. Acta 333, 85–94), which can recombine with an oxidizing equivalent in a state S₂ present in very small amount. As in photoinduced luminescence, this recombination excites chlorophyll which then emits light. A much stronger emission L_H is observed after injection of H₂O₂. Both signals are modified or suppressed by treatments specific of the oxygen emission system, such as: thermal denaturation at 50°C, NH₂OH, etc. In addition, a weak, permanent background luminescence L₀ has been observed; like L_D and L_H, it is a System II property and requires the integrity of the oxygen-evolving system. It is believed to reflect a very slow back flow of electrons from an endogeneous reductant pool to oxygen through part of the photosynthetic chain. Using flash preillumination, it is demonstrated that H₂O₂ is able to oxidize S₀ into S₂, the latter giving rise to L_H; H₂O₂ does not act on S₁ (or much less). The reactive site of H₂O₂ seems to be the same as the binding site of NH₂OH. Evidence is given that the strong L_H signal in particular reveals a stable, low pH of the intrathylakoid phase in Chlorella.