Reaction centers from three herbicide-resistant mutants of Rhodobacter sphaeroides 2.4.1: sequence analysis and preliminary characterization

Nano-mechanical mapping of the interactions between surface-bound RC-LH1-PufX core complexes and cytochrome c 2 attached to an AFM probe

Electron transfer pathways in photosynthesis involve interactions between membrane-bound complexes such as reaction centres with an extrinsic partner. In this study, the biological specificity of electron transfer between the reaction centre-light-harvesting 1-PufX complex and its extrinsic electron donor, cytochrome c 2, formed the basis for mapping the location of surface-attached RC-LH1-PufX complexes using atomic force microscopy (AFM). This nano-mechanical mapping method used an AFM probe functionalised with cyt c 2 molecules to quantify the interaction forces involved, at the single-molecule level under native conditions. With surface-bound RC-His12-LH1-PufX complexes in the photo-oxidised state, the mean interaction force with cyt c 2 is approximately 480 pN with an interaction frequency of around 66 %. The latter value lowered 5.5-fold when chemically reduced RC-His12-LH1-PufX complexes are imaged in the dark to abolish electron transfer from cyt c 2 to the RC. The correspondence between topographic and adhesion images recorded over the same area of the sample shows that affinity-based AFM methods are a useful tool when topology alone is insufficient for spatially locating proteins at the surface of photosynthetic membranes.

Evaluation of a biohybrid photoelectrochemical cell employing the purple bacterial reaction centre as a biosensor for herbicides

The Rhodobacter sphaeroides reaction centre is a relatively robust and tractable membrane protein that has potential for exploitation in technological applications, including biohybrid devices for photovoltaics and biosensing. This report assessed the usefulness of the photocurrent generated by this reaction centre adhered to a small working electrode as the basis for a biosensor for classes of herbicides used extensively for the control of weeds in major agricultural crops. Photocurrent generation was inhibited in a concentration-dependent manner by the triazides atrazine and terbutryn, but not by nitrile or phenylurea herbicides. Measurements of the effects of these herbicides on the kinetics of charge recombination in photo-oxidised reaction centres in solution showed the same selectivity of response. Titrations of reaction centre photocurrents yielded half maximal inhibitory concentrations of 208 nM and 2.1 µM for terbutryn and atrazine, respectively, with limits of detection estimated at around 8 nM and 50 nM, respectively. Photocurrent attenuation provided a direct measure of herbicide concentration, with no need for model-dependent kinetic analysis of the signal used for detection or the use of prohibitively complex instrumentation, and prospects for the use of protein engineering to develop the sensitivity and selectivity of herbicide binding by the Rba. sphaeroides reaction centre are discussed.

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The Rhodobacter sphaeroides reaction centre was used as a biosensor for herbicides.

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Herbicide concentration was assessed through the attenuation of a photocurrent.

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The biosensor showed selectivity for triazine herbicides.

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The limit of detection of the biosensor was in the low nanomolar range.

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Photocurrent attenuation is a simple and direct basis for a herbicide biosensor.

Bridging the gap: linking molecular simulations and systemic descriptions of cellular compartments

Metabolic processes in biological cells are commonly either characterized at the level of individual enzymes and metabolites or at the network level. Often these two paradigms are considered as mutually exclusive because concepts from neither side are suited to describe the complete range of scales. Additionally, when modeling metabolic or regulatory cellular systems, often a large fraction of the required kinetic parameters are unknown. This even applies to such simple and extensively studied systems like the photosynthetic apparatus of purple bacteria. Using the chromatophore vesicles of Rhodobacter sphaeroides as a model system, we show that a consistent kinetic model emerges when fitting the dynamics of a molecular stochastic simulation to a set of time dependent experiments even though about two thirds of the kinetic parameters in this system are not known from experiment. Those kinetic parameters that were previously known all came out in the expected range. The simulation model was built from independent protein units composed of elementary reactions processing single metabolites. This pools-and-proteins approach naturally compiles the wealth of available molecular biological data into a systemic model and can easily be extended to describe other systems by adding new protein or nucleic acid types. The automated parameter optimization, performed with an evolutionary algorithm, reveals the sensitivity of the model to the value of each parameter and the relative importances of the experiments used. Such an analysis identifies the crucial system parameters and guides the setup of new experiments that would add most knowledge for a systemic understanding of cellular compartments. The successful combination of the molecular model and the systemic parametrization presented here on the example of the simple machinery for bacterial photosynthesis shows that it is actually possible to combine molecular and systemic modeling. This framework can now straightforwardly be applied to other currently less well characterized but biologically more relevant systems.

Turnover of ubiquinone-0 at the acceptor side of photosynthetic reaction center

The steady-state operation of photosynthetic reaction center from Rhodobacter sphaeroides was investigated by measuring the rate of cytochrome photo-oxidation under intensive continuous illumination (808 nm, 5 W cm(-2)). The native quinone UQ10 in Q(B) binding site of the reaction center was substituted by tailless UQ0 and the binding parameters and the turnover rate of the UQ0 was studied to test the recently discovered light-intensity dependent acceptor side effect (Gerencsér and Maróti 2006). The binding parameters of UQ0 (k(on) = 2.1 x 10(5) M(-1) s(-1) and k(off) = 100 s(-1)) were characteristic to the RC exposed to high light-intensity. The dissociation constant (K (D) = 480 microM) determined under high light intensity is 2-3 times larger than that determined from flash-experiments. The light-intensity dependent acceleration of cytochrome turnover measured on reaction center of inhibited proton binding was independent of the type of the quinone and was sensitive only to the size ("pressure") of the quinone pool. The dissociation constants of different types of semiquinones show similarly high (several orders of magnitude) increase in the modified conformation of the Q(B) binding pocket due to high intensity of illumination. This result indicates the exclusive role of the quinone headgroup in the binding of semiquinone to different conformations of the protein.

ENDOR spectroscopy reveals light induced movement of the H-bond from Ser-L223 upon forming the semiquinone (Q(B)(-)(*)) in reaction centers from Rhodobacter sphaeroides

Proton ENDOR spectroscopy was used to monitor local conformational changes in bacterial reaction centers (RC) associated with the electron-transfer reaction DQB --> D+*QB-* using mutant RCs capable of photoreducing QB at cryogenic temperatures. The charge separated state D+*QB-* was studied in mutant RCs formed by either (i) illuminating at low temperature (77 K) a sample frozen in the dark (ground state protein conformation) or (ii) illuminating at room temperature prior to and during freezing (charge separated state protein conformation). The charge recombination rates from the two states differed greatly (>10(6) fold) as shown previously, indicating a structural change (Paddock et al. (2006) Biochemistry 45, 14032-14042). ENDOR spectra of QB-* from both samples (35 GHz, 77 K) showed several H-bond hyperfine couplings that were similar to those for QB-* in native RCs indicating that in all RCs, QB-* was located at the proximal position near the metal site. In contrast, one set of hyperfine couplings were not observed in the dark frozen samples but were observed only in samples frozen under illumination in which the protein can relax prior to freezing. This flexible H-bond was assigned to an interaction between the Ser-L223 hydroxyl and QB-* on the basis of its absence in Ser L223 --> Ala mutant RCs. Thus, part of the protein relaxation, in response to light induced charge separation, involves the formation of an H-bond between the OH group of Ser-L223 and the anionic semiquinone QB-*. These results show the flexibility of the Ser-L223 H-bond, which is essential for its function in proton transfer to reduced QB.

Monitoring the pH Dependence of IR Carboxylic Acid Signals upon QB- Formation in the Glu-L212 → Asp/Asp-L213 → Glu Swap Mutant Reaction Center from Rhodobacter sphaeroides

In the photosynthetic reaction center (RC) from the purple bacterium Rhodobacter sphaeroides, proton-coupled electron-transfer reactions occur at the secondary quinone (QB) site. Involved in the proton uptake steps are carboxylic acids, which have characteristic infrared vibrations in the 1770-1700 cm-1 spectral range that are sensitive to 1H/2H isotopic exchange. With respect to the native RC, a novel protonation pattern for carboxylic acids upon QB photoreduction has been identified in the Glu-L212 --> Asp/Asp-L213 --> Glu mutant RC using light-induced FTIR difference spectroscopy (Nabedryk, E., Breton, J., Okamura, M. Y., and Paddock, M. L. (2004) Biochemistry 43, 7236-7243). These carboxylic acids are structurally close and have been implicated in proton transfer to reduced QB. In this work, we extend previous studies by measuring the pH dependence of the QB-/QB FTIR difference spectra of the mutant in 1H2O and 2H2O. Large pH dependent changes were observed in the 1770-1700 cm-1 spectral range between pH 8 and pH 4. The IR fingerprints of the protonating carboxylic acids upon QB- formation were obtained from the calculated double-difference spectra 1H2O minus 2H2O. These IR fingerprints are specific for each pH, indicative of the contribution of different titrating groups. In particular, the 1752 cm-1 signal indicates that Glu-L213 protonates upon QB- formation at pH >or= 5, whereas the 1746 cm-1 signal indicates protonation of Asp-L212 even at pH 4. An unidentified carboxylic acid absorbing at approximately 1765 cm-1 could be the proton donor between pH 8 and 5. The observation that in the swap mutant there are several uniquely behaving carboxylic acids shows that electrostatic interactions occurring between them are sufficiently modified from the native RC to reveal their IR signatures.

Light induced EPR spectra of reaction centers from Rhodobacter sphaeroides at 80K: Evidence for reduction of Q(B) by B-branch electron transfer in native reaction centers

Photosynthetic reaction centers (RCs) from Rhodobacter sphaeroides capture solar energy by electron transfer from primary donor, D, to quinone acceptor, Q(B,) through the active A-branch of electron acceptors, but not the inactive B-branch. The light induced EPR spectrum from native RCs that had Fe(2+) replaced by Zn(2+) was investigated at cryogenic temperature (80K, 35 GHz). In addition to the light induced signal due to formation of D(+•)Q(A) (-•) observed previously, a small fraction (~5%) of the signal displayed very different characteristics: (1) The signal was absent in RCs in which the Q(B) was displaced by the inhibitor stigmatellin. (2) Its decay time (τ=6 s) was the same as observed for D(+•)Q(B) (-•) in mutant RCs lacking Q(A,) which is significantly slower than for D(+•)Q(A) (-•) (τ=30 ms). (3) Its EPR spectrum was identical to that of D(+•)Q(B) (-•). (4) The quantum efficiency for forming the major component of the signal was the same as that found for mutant RCs lacking Q(A) (Φ =0.2%) and was temperature independent. These results are explained by direct photochemical reduction of Q(B)via B-branch electron transfer in a small fraction of native RCs.

Trapped conformational states of semiquinone (D+*QB-*) formed by B-branch electron transfer at low temperature in Rhodobacter sphaeroides reaction centers

The reaction center (RC) from Rhodobacter sphaeroides captures light energy by electron transfer between quinones QA and QB, involving a conformational gating step. In this work, conformational states of D+*QB-* were trapped (80 K) and studied using EPR spectroscopy in native and mutant RCs that lack QA in which QB was reduced by the bacteriopheophytin along the B-branch. In mutant RCs frozen in the dark, a light induced EPR signal due to D+*QB-* formed in 30% of the sample with low quantum yield (0.2%-20%) and decayed in 6 s. A small signal with similar characteristics was also observed in native RCs. In contrast, the EPR signal due to D+*QB-* in mutant RCs illuminated while freezing formed in approximately 95% of the sample did not decay (tau >107 s) at 80 K (also observed in the native RC). In all samples, the observed g-values were the same (g = 2.0026), indicating that all active QB-*'s were located in a proximal conformation coupled with the nonheme Fe2+. We propose that before electron transfer at 80 K, the majority (approximately 70%) of QB, structurally located in the distal site, was not stably reducible, whereas the minority (approximately 30%) of active configurations was in the proximal site. The large difference in the lifetimes of the unrelaxed and relaxed D+*QB-* states is attributed to the relaxation of protein residues and internal water molecules that stabilize D+*QB-*. These results demonstrate energetically significant conformational changes involved in stabilizing the D+*QB-* state. The unrelaxed and relaxed states can be considered to be the initial and final states along the reaction coordinate for conformationally gated electron transfer.

Reconstruction of a kinetic model of the chromatophore vesicles from Rhodobacter sphaeroides

We present a molecular model of a chromatophore vesicle from Rhodobacter sphaeroides. These vesicles are ideal benchmark systems for molecular and systemic simulations, because they have been well studied, they are small, and they are naturally separated from their cellular environment. To set up a photosynthetic chain working under steady-state conditions, we compiled from the experimental literature the specific activities and geometries that have been determined for their constituents. This data then allowed defining the stoichiometries for all membrane proteins. This article contains the kinetic part of the reconstructed model, while the spatial reconstruction is presented in a companion article. By considering the transport properties of the Cytochrome c(2) and ubiquinone pools, we show that their size and oxidation states allow for an efficient buffering of the statistical fluctuations that arise from the small size of the vesicles. Stoichiometric and kinetic considerations indicate that a typical chromatophore vesicle of Rb. sphaeroides with a diameter of 45 nm should contain approximately five bc(1) monomers.

Uncoupling of electron and proton transfers in the photocycle of bacterial reaction centers under high light intensity

Photosynthetic reaction centers produce and export oxidizing and reducing equivalents in expense of absorbed light energy. The formation of fully reduced quinone (quinol) requires a strict (1:1) stoichiometric ratio between the electrons and H(+) ions entering the protein. The steady-state rates of both transports were measured separately under continuous illumination in the reaction center from the photosynthetic bacterium Rhodobacter sphaeroides. The uptake of the first proton was retarded by different methods and made the rate-limiting reaction in the photocycle. As expected, the rate constant of the observed proton binding remained constant (7 s(-)(1)), but that of the cytochrome photooxidation did show a remarkably large increase from 14 to 136 s(-)(1) upon increase of the exciting light intensity up to 5 W/cm(2) (808 nm) at pH 8.4 in the presence of NiCl(2). This corresponds to about 20:1 (e(-):H(+)) stoichiometric ratio. The observed enhancement is linearly proportional to the light intensity and the rate constant of the proton uptake by the acceptor complex and shows saturation character with quinone availability. For interpretation of the acceleration of cytochrome turnover, an extended model of the photocycle is proposed. A fraction of photochemically trapped RC can undergo fast (>10(3) s(-)(1)) conformational change where the semiquinone loses its high binding affinity (the dissociation constant increases by more than 5 orders of magnitude) and dissociates from the Q(B) binding site of the protein with a high rate of 4000 s(-)(1). Concomitantly, superoxide is being produced. No H(+) ion is taken up, and no quinol is created by the photocycle which is operating in about 25% of the reaction centers at the highest light intensity (5500 s(-)(1)) and slowest proton uptake (3.5 s(-)(1)) used in our experiments. The possible physical background of the light-induced conformational change and the relationship between the energies of dissociation and redox changes of the quinone in the Q(B) binding sites are discussed.

An Isotope-Edited FTIR Investigation of the Role of Ser-L223 in Binding Quinone (QB) and Semiquinone (QB-) in the Reaction Center from Rhodobacter sphaeroides

In the photosynthetic reaction center (RC) from the purple bacterium Rhodobacter sphaeroides, proton-coupled electron-transfer reactions occur at the secondary quinone (Q(B)) site. Several nearby residues are important for both binding and redox chemistry involved in the light-induced conversion from Q(B) to quinol Q(B)H(2). Ser-L223 is one of the functionally important residues located near Q(B). To obtain information on the interaction between Ser-L223 and Q(B) and Q(B)(-), isotope-edited Q(B)(-)/Q(B) FTIR difference spectra were measured in a mutant RC in which Ser-L223 is replaced with Ala and compared to the native RC. The isotope-edited IR fingerprint spectra for the C=O [see text] and C=C [see text] modes of Q(B) (Q(B)(-)) in the mutant are essentially the same as those of the native RC. These findings indicate that highly equivalent interactions of Q(B) and Q(B)(-) with the protein occur in both native and mutant RCs. The simplest explanation of these results is that Ser-L223 is not hydrogen bonded to Q(B) or Q(B)(-) but presumably forms a hydrogen bond to a nearby acid group, preferentially Asp-L213. The rotation of the Ser OH proton from Asp-L213 to Q(B)(-) is expected to be an important step in the proton transfer to the reduced quinone. In addition, the reduced quinone remains firmly bound, indicating that other distinct hydrogen bonds are more important for stabilizing Q(B)(-). Implications on the design features of the Q(B) binding site are discussed.

Quinone (QB) Reduction by B-Branch Electron Transfer in Mutant Bacterial Reaction Centers from Rhodobacter sphaeroides: Quantum Efficiency and X-ray Structure,

The photosynthetic reaction center (RC) from purple bacteria converts light into chemical energy. Although the RC shows two nearly structurally symmetric branches, A and B, light-induced electron transfer in the native RC occurs almost exclusively along the A-branch to a primary quinone electron acceptor Q(A). Subsequent electron and proton transfer to a mobile quinone molecule Q(B) converts it to a quinol, Q(B)H(2). We report the construction and characterization of a series of mutants in Rhodobacter sphaeroides designed to reduce Q(B) via the B-branch. The quantum efficiency to Q(B) via the B-branch Phi(B) ranged from 0.4% in an RC containing the single mutation Ala-M260 --> Trp to 5% in a quintuple mutant which includes in addition three mutations to inhibit transfer along the A-branch (Gly-M203 --> Asp, Tyr-M210 --> Phe, Leu-M214 --> His) and one to promote transfer along the B-branch (Phe-L181 --> Tyr). Comparing the value of 0.4% for Phi(B) obtained in the AW(M260) mutant, which lacks Q(A), to the 100% quantum efficiency for Phi(A) along the A-branch in the native RC, we obtain a ratio for A-branch to B-branch electron transfer of 250:1. We determined the structure of the most effective (quintuple) mutant RC at 2.25 A (R-factor = 19.6%). The Q(A) site did not contain a quinone but was occupied by the side chain of Trp-M260 and a Cl(-). In this structure a nonfunctional quinone was found to occupy a new site near M258 and M268. The implications of this work to trap intermediate states are discussed.

Specific Triazine Resistance in Bacterial Reaction Centers Induced by a Single Mutation in the QA Protein Pocket

We report here the first example of a reaction center mutant from Rhodobacter sphaeroides, where a single mutation (M266His --> Leu) taking place in the primary quinone protein pocket confers selective resistance to triazine-type inhibitors (terbutryn, ametryn, and atrazine), which bind in the secondary quinone protein pocket, at about 13 A from the mutation site. The M266His --> Leu mutation involves one of the iron atom ligands. Interestingly, neither the secondary quinone nor the highly specific inhibitor stigmatellin binding affinities are affected by the mutation. It is noticeable that in the M266His --> Ala mutant a nativelike behavior in observed. We suggest that the long side chain of Leu in position M266 may lack space to accommodate in the Q(A) pocket therefore transferring its hindrance to the Q(B) pocket. This may occur via the structural feature formed by the Q(A)-M219His-Fe-L190His-inhibitor (or Q(B)) connection, pushing L189Leu and/or L229Ile in closer contact to the triazine molecules, therefore decreasing their bindings. This opens the possibility to finely tune, in reaction center proteins, the affinity for herbicides by designing mutations distant from their binding sites.

NMR Structural Model of the Interaction of Herbicides with the Photosynthetic Reaction Center from Rhodobacter sphaeroides

The interaction of the herbicides acifluorfen and paraquat with the photosynthetic reaction center from Rhodobacter sphaeroides has been studied by NMR relaxation measurements. Interaction in aqueous solution has been demonstrated by evaluating motional features of the bound form through cross-relaxation terms of protons at fixed distances on the herbicides. Contributions to longitudinal nonselective relaxation rates different from the proton-proton dipolar relaxation were inferred, most probably due to paramagnetic effects originating from the high-spin nonheme Fe(II) ion in the reaction center. Paramagnetic contributions to proton relaxation rates were converted into distance constraints in order to build a model for the interaction. The models place paraquat in the QB site, where most herbicides interact, in agreement with docking calculations, whereas acifluorfen was placed between the metal and the QB site, as also demonstrated by the induced paramagnetic shifts. Acifluorfen could therefore act to break the electron-transfer pathway between the QA and QB sites.

Identification of a Novel Protonation Pattern for Carboxylic Acids upon QB Photoreduction in Rhodobacter sphaeroides Reaction Center Mutants at Asp-L213 and Glu-L212 Sites

In the reaction center from the photosynthetic purple bacterium Rhodobacter sphaeroides, light energy is rapidly converted to chemical energy through coupled electron-proton transfer to a buried quinone molecule Q(B). Involved in the proton uptake steps are carboxylic acids, which have characteristic infrared vibrations that are observable using light-induced Fourier transform infrared (FTIR) difference spectroscopy. Upon formation, Q(B)(-) induces protonation of Glu-L212, located within 5 A of Q(B), resulting in a IR signal at 1728 cm(-1). However, no other IR signal is observed within the classic absorption range of protonated carboxylic acids (1770-1700 cm(-1)). In particular, no signal for Asp-L213 is found despite its juxtaposition to Q(B) and importance for proton uptake on the second electron-transfer step. In an attempt to uncover the reason behind this lack of signal, the microscopic electrostatic environment in the vicinity of Q(B) was modified by interchanging Asp and Glu at the L213 and L212 positions. The Q(B)(-)/Q(B) FTIR spectrum of the Asp-L212/Glu-L213 swap mutant in the 1770-1700 cm(-1) range shows several distinct new signals, which are sensitive to (1)H/(2)H isotopic exchange, indicating that the reduction of Q(B) results in the change of the protonation state of several carboxylic acids. The new bands at 1752 and 1747 cm(-1) were assigned to an increase of protonation in response to Q(B) reduction of Glu-L213 and Asp-L212, respectively, based on the effect of replacing them with their amine analogues. Since other carboxylic acid signals were observed, it is concluded that the swap mutations at L212 and L213 affect a cluster of carboxylic acids larger than the L212/L213 acid pair. Implications for the native reaction center are discussed.

X-Ray Structure Determination of Three Mutants of the Bacterial Photosynthetic Reaction Centers from Rb. sphaeroides

In the photosynthetic reaction center (RC) from Rhodobacter sphaeroides, the reduction of a bound quinone molecule Q(B) is coupled with proton uptake. When Asp-L213 is replaced by Asn, proton transfer is inhibited. Proton transfer was restored by two second-site revertant mutations, Arg-M233-->Cys and Arg-H177-->His. Kinetic effects of Cd(2+) on proton transfer showed that the entry point in revertant RCs to be the same as in the native RC. The structures of the parental and two revertant RCs were determined at resolutions of 2.10, 1.80, and 2.75 A. From the structures, we were able to delineate alternate proton transfer pathways in the revertants. The main changes occur near Glu-H173, which allow it to substitute for the missing Asp-L213. The electrostatic changes near Glu-H173 cause it to be a good proton donor and acceptor, and the structural changes create a cavity which accommodates water molecules that connect Glu-H173 to other proton transfer components.

Absorption changes induced by the binding of triazines to the QB pocket in reaction centers of Rhodobacter capsulatus

Inhibitors which block electron transfer from the primary (Q(A)) to the secondary (Q(B)) quinone of the bacterial reaction center are competing with the pool ubiquinones for binding at the Q(B) pocket. Due to the much greater stability of the semiquinone state Q(B)(-) compared with fully oxidized or reduced quinone, a displacement of the inhibitors takes place after one flash from state Q(A)(-)I to state Q(A)Q(B)(-). This process can be monitored from near-IR absorption changes which reflect local absorption shifts specific to Q(A)(-) and Q(B)(-). An anomalous behavior was observed when using triazines in chromatophores of R. capsulatus: the IR absorption change reflecting the formation of Q(B)(-) after one flash was absent. A normal transient decay of this signal was, however, triggered by a second flash, followed by a rapid return to the baseline. We show that this phenomenon is due to an absorption change induced by inhibitor binding (thus present in the dark baseline), with a spectrum close to that of Q(B)(-), so that the Q(B)(-) changes are canceled out during the inhibitor displacement process. On the second flash, one monitors the destruction of the semiquinone, leading transiently to the Q(A)Q(B) state, followed by inhibitor rebinding. This allows a direct measurement of the binding kinetics. This behavior was observed both in chromatophores and in isolated reaction centers from R. capsulatus, but not in R. sphaeroides.

Cloning and sequencing of glycogen metabolism genes from Rhodobacter sphaeroides 2.4.1. Expression and characterization of recombinant ADP-glucose pyrophosphorylase

A 6-kb DNA fragment of the Rhodobacter sphaeroides 2.4.1 glg operon was cloned from a genomic library using a polymerase chain reaction probe coding for part of the ADP-glucose pyrophosphorylase (glgC) gene. The DNA fragment was sequenced and found to harbor complete open reading frames for the glgC and glgA (glycogen synthase) genes and partial sequences corresponding to glgP (glycogen phosphorylase) and glgX (glucan hydrolase/transferase) genes. The genomic fragment also contained an apparent truncated sequence corresponding to the C-terminus of the glgB gene (branching enzyme). The presence of active branching enzyme activity in crude sonicates of Rb. sphaeroides cells indicates that the genome contains a full-length glgB at another location. The structure of this operon in relation to other glg operons is further discussed. The deduced sequence of the ADP-glucose pyrophosphorylase enzyme is compared to other known ADP-glucose pyrophosphorylase sequences and discussed in relation to the allosteric regulation of this enzyme family. The glgC gene was subcloned in the vector pSE420 (Invitrogen) for high-level expression in E. coli. The successful overexpression of the recombinant enzyme allowed for the purification of over 35 mg of protein from 10 g of cells, representing a dramatic improvement over enzyme isolation from the native strain. The recombinant enzyme was purified to near homogeneity and found to be physically, immunologically, and kinetically identical to the native enzyme, verifying the fidelity of the cloning step.

Characterization of ADP-glucose pyrophosphorylase from Rhodobacter sphaeroides 2.4.1: evidence for the involvement of arginine in allosteric regulation

ADP-glucose pyrophosphorylase (ADPGlc PPase, EC 2.7.7.27) from Rhodobacter sphaeroides 2.4.1 has been purified to near homogeneity. The enzyme reacted in Western blots to polyclonal antibodies raised against other bacterial ADPGlc PPases. The purified enzyme was found to be activated by fructose 6-phosphate, fructose 1,6-bisphosphate, and pyruvate and inhibited by phosphate, phosphoenolpyruvate, ADP, and pyridoxal phosphate. Kinetic studies indicate that AMP, while having little effect on kinetic parameters at pH 8 in the absence of effectors, is a specific ligand for an allosteric site(s). Treatment of the purified enzyme with the arginyl reagents 2,3-butanedione and phenylglyoxal resulted in desensitization of the enzyme to both activation and inhibition by metabolites. Phosphate, fructose 6-phosphate, and AMP were found to protect the enzyme against allosteric desensitization supportive of these metabolites interacting at common site(s) or with a common enzyme form. As a first step in cloning the gene coding for this enzyme, a polymerase chain reaction fragment was generated from genomic DNA using primers based on amino terminal sequencing data and a highly conserved region in known ADPGlc PPases. The sequence of this fragment and position of amino terminal arginines in comparison to other known ADPGlc PPases is discussed in relation to the kinetic and chemical modification data.

Excited-state electronic asymmetry of the special pair in photosynthetic reaction center mutants: absorption and Stark spectroscopy

The electronic absorption line shape and Stark spectrum of the lowest energy Q(y)() transition of the special pair in bacterial reaction centers contain a wealth of information on mixing with charge transfer states and electronic asymmetry. Both vary greatly in mutants that perturb the chemical composition of the special pair, such as the heterodimer mutants, and in mutants that alter interactions between the special pair and the surrounding reaction center protein, such as those that add or remove hydrogen bonds. The conventional and higher-order Stark spectra of a series of mutants are presented with the aim of developing a systematic description of the electronic structure of the excited state of the special pair that initiates photosynthetic charge separation. The mutants L168HF, M197FH, L131LH and L131LH/M160LH/M197FH are known to have different hydrogen-bonding patterns to the special pair; however, they exhibit Stark effects that are very similar to wild type. By contrast, the addition of a hydrogen bond to the M-side keto carbonyl group of the special pair in M160LH greatly affects both the absorption and Stark spectra. The heterodimer special pairs, L173HL and M202HL, exhibit much larger Stark effects than wild type, with the greatest effect in the M-side mutant. Double mutants that combine the M-side heterodimer and a hydrogen-bond addition to the L-side of the special pair decrease the magnitude of the Stark effect. These results suggest that the electronic asymmetry of the dimer can be perturbed either by the formation of a heterodimer or by adding or deleting a hydrogen bond to a keto carbonyl group. From the pattern observed, it is concluded that the charge transfer state P(L)(+)P(M)(-) has a larger influence on the excited state of the dimer in wild type than the P(L)(-)P(M)(+)charge transfer state. Furthermore, asymmetry can be varied continuously, from extreme cases in which the heterodimer and hydrogen-bond effects work together, to cases in which hydrogen bonding offsets the effects of the heterodimer, to cases in which the homodimer is perturbed by hydrogen bonds. This leads to a unified model for understanding the effects of perturbations on the electronic symmetry of the special pair, and this can be connected with perturbations on the properties of many other systems such as donor-acceptor-substituted polyenes.

Observation of the protonated semiquinone intermediate in isolated reaction centers from Rhodobacter sphaeroides: implications for the mechanism of electron and proton transfer in proteins

A proton-activated electron transfer (PAET) mechanism, involving a protonated semiquinone intermediate state, had been proposed for the electron-transfer reaction k(2)AB [Q(A)(-)(*)Q(B)(-)(*) + H(+) <--> Q(A)(-)(*)(Q(B)H)(*) --> Q(A)(Q(B)H)(-)] in reaction centers (RCs) from Rhodobacter sphaeroides [Graige, M. S., Paddock, M. L., Bruce, M. L., Feher, G., and Okamura, M. Y. (1996) J. Am. Chem. Soc. 118, 9005-9016]. Confirmation of this mechanism by observing the protonated semiquinone (Q(B)H)(*) had not been possible, presumably because of its low pK(a). By replacing the native Q(10) in the Q(B) site with rhodoquinone (RQ), which has a higher pK(a), we were able to observe the (Q(B)H)(*) state. The pH dependence of the semiquinone optical spectrum gave a pK(a) = 7.3 +/- 0.2. At pH < pK(a), the observed rate for the reaction was constant and attributed to the intrinsic electron-transfer rate from Q(A)(-)(*) to the protonated semiquinone (i.e., k(2)AB = k(ET)(RQ) = 2 x 10(4) s(-)(1)). The rate decreased at pH > pK(a) as predicted by the PAET mechanism in which fast reversible proton transfer precedes rate-limiting electron transfer. Consequently, near pH 7, the proton-transfer rate k(H) >> 10(4) s(-)(1). Applying the two step mechanism to RCs containing native Q(10) and taking into account the change in redox potential, we find reasonable values for the fraction of (Q(B)H)(*) congruent with 0.1% (consistent with a pK(a)(Q(10)) of approximately 4.5) and k(ET)(Q(10)) congruent with 10(6) s(-)(1). These results confirm the PAET mechanism in RCs with RQ and give strong support that this mechanism is active in RCs with Q(10) as well.

Conformational gating of the electron transfer reaction QA-.QB --> QAQB-. in bacterial reaction centers of Rhodobacter sphaeroides determined by a driving force assay

The mechanism of the electron transfer reaction, QA-.QB --> QAQB-., was studied in isolated reaction centers from the photosynthetic bacterium Rhodobacter sphaeroides by replacing the native Q10 in the QA binding site with quinones having different redox potentials. These substitutions are expected to change the intrinsic electron transfer rate by changing the redox free energy (i.e., driving force) for electron transfer without affecting other events that may be associated with the electron transfer (e.g., protein dynamics or protonation). The electron transfer from QA-. to QB was measured by three independent methods: a functional assay involving cytochrome c2 to measure the rate of QA-. oxidation, optical kinetic spectroscopy to measure changes in semiquinone absorption, and kinetic near-IR spectroscopy to measure electrochromic shifts that occur in response to electron transfer. The results show that the rate of the observed electron transfer from QA-. to QB does not change as the redox free energy for electron transfer is varied over a range of 150 meV. The strong temperature dependence of the observed rate rules out the possibility that the reaction is activationless. We conclude, therefore, that the independence of the observed rate on the driving force for electron transfer is due to conformational gating, that is, the rate limiting step is a conformational change required before electron transfer. This change is proposed to be the movement, controlled kinetically either by protein dynamics or intermolecular interactions, of QB by approximately 5 A as observed in the x-ray studies of Stowell et al. [Stowell, M. H. B., McPhillips, T. M., Rees, D. C., Soltis, S. M., Abresch, E. & Feher, G. (1997) Science 276, 812-816].

Proton and electron transfer to the secondary quinone (QB) in bacterial reaction centers: the effect of changing the electrostatics in the vicinity of QB by interchanging asp and glu at the L212 and L213 sites

The bacterial reaction center (RC) plays a central role in photosynthetic energy conversion by facilitating the light induced double reduction and protonation of a bound quinone molecule, QB. Two carboxylic acid residues, Asp-L213 and Glu-L212, located near QB, were previously shown to be important for proton transfer to QB. In this work, the ability of Glu to substitute for Asp at L213 and Asp to substitute for Glu at L212 was tested by site-directed mutagenesis. Both single mutants and a double mutant in which Asp and Glu were exchanged between the two sites were constructed. The electron transfer rate constants kBD (D+QAQB- --> DQAQB), and kAB(2) (DQA-QB- + H+ --> DQA(QBH)-), that are known to be sensitive to the energy of the QB- state, were found to be altered by Asp/Glu substitutions. Both rates were fastest ( approximately 10-fold) in RCs with Asp at both sites, slowest with Glu at both sites ( approximately 50-fold) and relatively unchanged by the caboxylic acid exchange. These changes could be explained if Asp was predominantly ionized and Glu was predominantly protonated at both sites (pH 7.5). The charge recombination kBD suggests an observed approximately 5 pKa unit difference of Glu over Asp. Modeling of kBD by strong electrostatic interactions ( approximately 3-4 pKa units) among negatively charged acids and QB- indicated a lower intrinsic pKa for Asp compared to Glu at either site of approximately 2-3 units. The mechanism of the kAB(2) reaction was determined to be the same in all mutant RCs as for native RCs. A quantitative explanation of the effect of the electrostatic environment on kAB(2) was obtained using the two-step model proposed for native RCs [Graige, M. S., Paddock, M. L., Bruce, J. M., Feher, G., & Okamura, M. Y. (1996) J. Am. Chem. Soc. 118, 9005-9016] which involves fast protonation of the semiquinone followed by rate-limiting electron transfer. Using simple models for the quinone/quinol conversion rate, it is shown that the optimal electrostatic potential for the QB site is close to that found in native RCs.

The coupling of light-induced electron transfer and proton uptake as derived from crystal structures of reaction centres from Rhodopseudomonas viridis modified at the binding site of the secondary quinone, QB

BACKGROUND

In a reaction of central importance to the energetics of photosynthetic bacteria, light-induced electron transfer in the reaction centre (RC) is coupled to the uptake of protons from the cytoplasm at the binding site of the secondary quinone (QB). In the original structure of the RC from Rhodopseudomonas viridis (PDB entry code 1PRC), the QB site was poorly defined because in the standard RC crystals it was only approximately 30% occupied with ubiquinone-9 (UQ9). We report here the structural characterization of the QB site by crystallographic refinement of UQ9-depleted RCs and of complexes of the RC either with ubiquinone-2 (UQ2) or the electron-transfer inhibitor stigmatellin in the QB site.

RESULTS

The structure of the RC complex with UQ2, refined at 2.45 A resolution, constitutes the first crystallographically reliably defined binding site for quinones from the bioenergetically important quinone pool of biological, energy-transducing membranes. In the UQ9-depleted QB site of the RC structure, refined at 2.4 A resolution, apparently five (and possibly six) water molecules are bound instead of the ubiquinone head group, and a detergent molecule binds in the region of the isoprenoid tail. All of the protein-cofactor interactions implicated in the binding of the ubiquinone head group are also implicated in the binding of the stigmatellin head group. In the structure of the stigmatellin-RC complex, refined at 2.4 A resolution, additional hydrogen bonds stabilize the binding of stigmatellin over that of ubiquinone. The tentative position of UQ9 in the QB site in the original data set (1PRC) was re-examined using the structure of the UQ9-depleted RC as a reference. A modified QB site model, which exhibits greater similarity to the distal ubiquinone-10 (UQ10) positioning in the structure of the RC from Rhodobacter sphaeroides (PDB entry code 1PCR), is suggested as the dominant binding site for native UQ9.

CONCLUSIONS

The structures reported here can provide models of quinone reduction cycle intermediates. The binding pattern observed for the stigmatellin complex, where the ligand donates a hydrogen bond to Ser L223 (where 'L' represents the L subunit of the RC), can be viewed as a model for the stabilization of a monoprotonated reduced intermediate (QBH or QBH-). The presence of Ser L223 in the QB site indicates that the QB site is not optimized for QB binding, but for QB reduction to the quinol.

Reduced turnover of the D1 polypeptide and photoactivation of electron transfer in novel herbicide resistant mutants of Synechocystis sp. PCC 6803

Two missense mutants, A263P and S264P, and a deletion mutant des-Ala263, Ser264, have been constructed in the D1 protein of the cyanobacterium Synechocystis sp PCC 6803. All were expected to induce a significant conformational change in the QB-binding region of photosystem II (PSII). Although the des-Ala263, Ser264-D1 mutant accumulated some D1 protein in the thylakoid membrane it was unable to grow photoautotrophically or evolve oxygen. Thermoluminescence and chlorophyll fluorescence studies confirmed that this deletion mutant did not show any functional PSII activity. In contrast, [S264P]D1 was able to grow photoautotrophically and give light-saturated rates of oxygen evolution at 60% of the rate of the wild-type control strain, TC31. The A263P missense mutant was also able to evolve oxygen at 50% of TC31 rates although it did not readily grow photoautotrophically. Thermoluminescence, flash oxygen yield and chlorophyll fluorescence measurements indicated that in both missense mutants electron transfer from QA to QB was significantly impaired in dark adapted cells. However, QA to QB electron transfer could be photoactivated in the mutants by background illumination. Both the A263P and S264P mutants also showed an increase in resistance to the s-triazine family of herbicides although this feature did not hold for the phenolic herbicide, ioxynil. Of particular interest was that the two missense mutants, especially S264P, possessed a slower rate of turnover of the D1 protein compared with TC31 and in vivo contained detectable levels of a 41-kDa adduct consisting of D1 and the alpha subunit of cytochrome b559. When protein synthesis was blocked by the addition of lincomycin, D1 degradation was again slower in S264P than TC31. The results are discussed in terms of structural changes in the QB-binding region which affect herbicide and plastoquinone binding and perturb the normal regulatory factors that control the degradation of the D1 protein and its synchronisation with the synthesis of a replacement D1 protein.

Resistance of reaction centers from Rhodobacter sphaeroides against UV-B radiation. Effects on protein structure and electron transport

Inhibition of electron transport and damage to the protein subunits by ultraviolet-B (UV-B, 280-320 nm) radiation have been studied in isolated reaction centers of the non-sulfur purple bacterium Rhodobacter sphaeroides R26. UV-B irradiation results in the inhibition of charge separation as detected by the loss of the initial amplitude of absorbance change at 430 nm reflecting the formation of the P(+)(QAQB)(-) state. In addition to this effect, the charge recombination accelerates and the damping of the semiquinone oscillation increases in the UV-B irradiated reaction centers. A further effect of UV-B is a 2 fold increase in the half- inhibitory concentration of o-phenanthroline. Some damage to the protein subunits of the RC is also observed as a consequence of UV-B irradiation. This effect is manifested as loss of the L, M and H subunits on Coomassie stained gels, but not accompanied with specific degradation products. The damaging effects of UV-B radiation enhanced in reaction centers where the quinone was semireduced (QB (-)) during UV-B irradiation, but decreased in reaction centers which lacked quinone at the QB binding site. In comparison with Photosystem II of green plant photosynthesis, the bacterial reaction center shows about 40 times lower sensitivity to UV-B radiation concerning the activity loss and 10 times lower sensitivity concerning the extent of reaction center protein damage. It is concluded that the main effect of UV-B radiation in the purple bacterial reaction center occurs at the QAQB quinone acceptor complex by decreasing the binding affinity of QB and shifting the electron equilibration from QAQB (-) to QA (-)QB. The inhibitory effect is likely to be caused by modification of the protein environment around the QB binding pocket and mediated by the semiquinone form of QB. The UV-resistance of the bacterial reaction center compared to Photosystem II indicates that either the QAQB acceptor complex, which is present in both types of reaction centers with similar structure and function, is much less susceptible to UV damage in purple bacteria, or, more likely, that Photosystem II contains UV-B targets which are more sensitive than its quinone complex.

Mg coordination by amino acid side chains is not required for assembly and function of the special pair in bacterial photosynthetic reaction centers

A conserved histidine serves as the axial ligand to the Mg of bacteriochlorophylls in the photosynthetic reaction center (RC) and many other photosynthetic systems. The histidine axial ligands to each and both bacteriochlorophylls of the special-pair primary electron donor of the Rhodobacter sphaeroides RC have been replaced with glycine to create a cavity. In each case, RCs assemble and a normal special-pair comprised of Mg-containing bacteriochlorophylls is formed, as judged by many different spectroscopic and functional probes (e.g., absorption and Stark spectra, *P decay kinetics, P+Q(A)- recombination rate, and the redox potential of P). In contrast with heme proteins, where this strategy has been exploited to introduce exogenous organic ligands that can greatly affect the functional properties of the protein [DePillis, G. D., Decatur, S. M., Barrick, D., & Boxer, S. G. (1994) J. Am. Chem. Soc. 116, 6981-6982], addition of exogenous imidazole, pyridine, and ethanethiol has no measurable effect on the functional properties of the special pair in these cavity mutants. FT-Raman spectroscopy is used to provide more detailed information on local interactions around the special pair. Data in the core-size marker mode and carbonyl stretching region suggest that an adventitious ligand replaces histidine as the axial ligand to bacteriochlorophylls in the cavity mutants. We speculate that this ligand is water. Furthermore, the position of the core-size marker mode changes when the cavity mutant RCs are incubated with exogenous ligands such as imidazole, pyridine, or ethanethiol, suggesting that the axial ligand to the special pair BChls can be exchanged in the cavity mutants. Interestingly the temperature dependence of P+Q(A)- recombination kinetics is very similar in the cavity mutants and WT, suggesting that the axial ligands to the special pair are not significant contributors to the solvent reorganization energy for this reaction. These results lead to the surprising conclusion that the nature of the axial ligand to the special pair has little influence on the properties of the macrocycle, and that axial coordination from the protein by histidine is not required for bacteriochlorophyll binding or for efficient electron transfer in the RC.

A new mutation in the pufL gene responsible for the terbutryn resistance phenotype in Rubrivivax gelatinosus

Rubrivivax gelatinosus is a facultative phototrophic non-sulfur bacterium belonging to the beta subclass of the purple bacteria. A terbutryn-resistant mutant of R. gelatinosus has been isolated and characterized. Increased resistance levels to terbutryn (300-fold), atrazine (6-fold) and o-phenanthroline (3-fold) were observed for the mutant compared with wild type. Sequence analysis of the mutant revealed a new mutation in the pufL gene coding for the L subunit of the reaction centre (RC) at codon 192 leading to an amino-acid substitution from Gly in the wild type to Asp in the mutant. This substitution is located in the D helix of the L subunit, suggesting an interaction between terbutryn and this part of the polypeptide in the RC of R. gelatinosus. This is the first report of a mutation leading to herbicide resistance and affecting the D helix in purple bacteria. Furthermore R. gelatinosus wild type is highly sensitive to o-phenanthroline compared with other purple bacteria (Rhodobacter capsulatus and Rhodobacter sphaeroides). Sequence comparison of the L subunit from six purple bacteria in which o-phenanthroline sensitivity was measured suggests that SerL226 might be responsible for this phenotype.

The Ile(L229) → Met mutation impairs the quinone binding to the QB-pocket in reaction centers of Rhodobacter sphaeroides

A spontaneous mutant (R/89) of photosynthetic purple bacterium Rhodobacter sphaeroides R-26 was selected for resistance to 200 μM atrazin. It showed increased resistance to interquinone electron transfer inhibitors of o-phenanthroline (resistance factor, RF=20) in UQo reconstituted isolated reaction centers and terbutryne in reaction centers (RF=55) and in chromatophores (RF=85). The amino acid sequence of the QB binding protein of the photosynthetic reaction center (the L subunit) was determined by sequencing the corresponding pufL gene and a single mutation was found (Ile(L229) → Met). The changed amino acid of the mutant strain is in van der Waals contact with the secondary quinone QB. The binding and redox properties of QB in the mutant were characterized by kinetic (charge recombination) and multiple turnover (cytochrome oxidation and semiquinone oscillation) assays of the reaction center. The free energy for stabilization of QAQB (-) with respect to QA (-)QB was ΔGAB=-60 meV and 0 meV in reaction centers and ΔGAB=-85 meV and -46 meV in chromatophores of R-26 and R/89 strains at pH 8, respectively. The dissociation constants of the quinone UQo and semiquinone UQo (-) in reaction centers from R-26 and R/89 showed significant and different pH dependence. The observed changes in binding and redox properties of quinones are interpreted in terms of differential effects (electrostatics and mesomerism) of mutation on the oxidized and reduced states of QB.

Modeling the quinone-B binding site of the photosystem-II reaction center using notions of complementarity and contact-surface between atoms

Functional identity and significant similarities in cofactors and sequence exist between the L and M reaction center proteins of the photosynthetic bacteria and the D1 and D2 photosystem-II reaction center proteins of cyanobacteria, algae, and plants. A model of the quinone (QB) binding site of the D1 protein is presented based upon the resolved structure of the QB binding pocket of the L subunit, and introducing novel quantitative notions of complementarity and contact surface between atoms. This model, built without using traditional methods of molecular mechanics and restricted to residues in direct contact with QB, accounts for the experimentally derived functional state of mutants of the D1 protein in the region of QB. It predicts the binding of both the classical and phenol-type PSII herbicides and rationalizes the relative levels of tolerance of mutant phenotypes.

Effect of ethoxyformic anhydride on the Rieske iron-sulfur protein of bovine heart ubiquinol: cytochrome c oxidoreductase

Treatment of bovine heart ubiquinol-cytochrome c oxidoreductase (complex III, bc1 complex) with ethoxyformic anhydride (EFA) inhibits electron transfer between cytochromes b and c1 [Yagi et al., Biochemistry 21 (1982) 4777-4782]. This paper shows that EFA alters the EPR lineshape of the Rieske iron-sulfur cluster in complex III and in the isolated Rieske protein without a significant decrease of spin concentration. The effect of EFA on the Rieske iron-sulfur cluster is competitive with that of Qo site inhibitors, such as stigmatellin, and is completely reversed by hydroxylamine. These results are consistent with the possible ethoxyformylation by EFA of histidine ligands of the Rieske iron-sulfur cluster at the non-iron binding imidazole nitrogens.

Pathway of proton transfer in bacterial reaction centers: role of aspartate-L213 in proton transfers associated with reduction of quinoneto dihydroquinone

The role of Asp-L213 in proton transfer to reduced quinone QB in the reaction center (RC) from Rhodobacter sphaeroides was studied by site-directed replacement of Asp with residues having different proton donor properties. Reaction centers (RCs) with Asn, Leu, Thr, and Ser at L213 had greatly reduced (approximately 6000-fold) proton-coupled electron transfer [kAB(2)] and proton uptake rates associated with the second electron reduction of QB (QA- QB- + 2H(+)-->QAQBH2) compared to native RCs. RCs containing Glu at L213 showed faster (approximately 90-fold) electron and proton transfer rates than the other mutant RCs but were still reduced (approximately 70-fold) compared with native RCs. These results show that kAB(2) is larger when a carboxylic acid occupies the L213 site, consistent with the proposal that Asp-L213 is a component of a proton transfer chain. The reduced kAB(2) observed with Glu versus Asp at L213 suggests that Asp at L213 is important for proton transfer for some other reason in addition to its proton transfer capabilities. Glu-L213 is estimated to have a higher apparent pKa (pKa > or = 7) than Asp-L213 (pKa < or = 4), as indicated by the slower rate of charge recombination (D+QAQB(-)-->DQAQB) in the mutant RCs. The importance of the pKa and charge of the residue at L213 for proton transfer are discussed. Based on these studies, a model for proton transfer is proposed in which Asp-L213 contributes to proton transfer in native RCs in two ways: (1) it is a component of a proton transfer chain connecting the buried QB molecule with the solvent and/or (2) it provides a negative charge that stabilizes a proton on or near QB.

Light-induced proton uptake by photosynthetic reaction centers from Rhodobacter sphaeroides R-26.1. II. Protonation of the state DQAQB2-

Proton uptake associated with the two-electron reduction of QB was investigated in reaction centers (RCs) from Rhodobacter sphaeroides R-26.1 using pH-sensitive dyes. An uptake of two protons was observed at pH < or = 7.5, consistent with the formation of the dihydroquinone QBH2. At higher pH, the proton uptake decreased with an apparent pKa of approx. 8.5, i.e., to 1.5 H+/2 e- at pH 8.5. A molecular model is presented in which the apparent pKa is due to the protonation of either the carbonyl oxygen on QB or of an amino acid residue near QB (e.g., His-L190). Experimental evidence in favor of the protonation of the oxygen is discussed. The kinetics of the electron transfer from QA-QB- to QAQB2- and the associated proton uptake were compared at several pH values and temperatures. At pH 8.5 (21.5 degrees C) the rate constants for the proton uptake and electron transfer are the same within the precision of the measurement. At lower pH, the proton uptake rate constant is smaller than that for electron transfer. The difference between the rate constants is temperature dependent, i.e., it varies from 12 +/- 4% at 21.5 degrees C (pH 7.5) to 28 +/- 4% at 4.0 degrees C (pH 7.5). We show that the kinetics can be explained by a previously proposed model (Paddock, M. L., McPherson, P. H., Feher, G. and Okamura, M. Y. (1990) Proc. Natl. Acad. Sci. USA 87, 6803-6807) in which the uptake of two protons by doubly reduced QB occurs sequentially, one concomitant with and the other after electron transfer.

Flash-induced proton transfer in photosynthetic bacteria

A proton electrochemical potential across the membranes of photosynthetic purple bacteria is established by a light-driven proton pump mechanism: the absorbed light in the reaction center initiates electron transfer which is coupled to the vectorial displacement of protons from the cytoplasm to the periplasm. The stoichiometry and kinetics of proton binding and release can be tracked directly by electric (glass electrodes), spectrophotometric (pH indicator dyes) and conductimetric techniques. The primary step in the formation of the transmembrane chemiosmotic potential is the uptake of two protons by the doubly reduced secondary quinone in the reaction center and the subsequent exchange of hydroquinol for quinone from the membrane quinone-pool. However, the proton binding associated with singly reduced promary and/or secondary quinones of the reaction center is substoichiometric, pH-dependent and its rate is electrostatically enhanced but not diffusion limited. Molecular details of protonation are discussed based on the crystallographic structure of the reaction center of purple bacteriaRb. sphaeroides andRps. viridis, structure-based molecular (electrostatic) calculations and mutagenesis directed at protonatable amino acids supposed to be involved in proton conduction pathways.

Reaction centers from three herbicide resistant mutants of Rhodobacter sphaeroides 2.4.1: Kinetics of electron transfer reactions

Electron transfer rates were measured in RCs from three herbicide-resistant mutants with known amino acid changes to elucidate the structural requirements for last electron transfer. The three herbicide resistant mutants were IM(L229) (Ile-L229↦ Met), SP(L223) (Ser-L223↦ Pro) and YG(L222) (Tyr-L222↦ Gly). The electron transfer rate D(+)QA (-)QB↦D(+)QAQB (k AB) is slowed ∼3 fold in the IM(L229) and YG(L222) RCs (pH 8). The stabilization of D(+)QAQB (-) with respect to D(+)QAQB (-) (pH 8) was found to be eliminated in the IM(L229) mutant RCs (ΔG(0) ∼ 0 meV), was partially reduced in the SP(L223) mutant RCs (ΔG(0)=-30 meV), and was unaltered in the YG(L222) mutant RCs (ΔG(0)=-60 meV), compared to that observed in the native RCs (ΔG(0)=-60 meV). The pH dependences of the charge recombination rate D(+)QAQB (-)↦DQAQB (k BD) and the electron transfer from QA (-) (k QA (-)↦QA) suggest that the mutations do not affect the protonation state of Glu-L212 nor the electrostatic interactions of QB and QB (-) with Glu-L212. The binding affinities of UQ10 for the QB site were found in order of decreasing values to be native ≥IM(L229) > YG(L222)≥ SP(L223). The altered properties of the mutant RCs are used to deduce possible structural changes caused by the mutations and are dicscussed in terms of photosynthetic efficiency of the herbicide resistant strains.

Characterization of Naturally Occurring Atrazine-Resistant Isolates of the Purple Non-Sulfur Bacteria

Six isolates of the purple non-sulfur bacteria, which upon primary isolation were naturally resistant to the herbicide atrazine, were characterized with respect to their taxonomic identity and the mechanism of their resistance. On the basis of electron microscopy, photopigment analysis, and other criteria, they were identified as strains of Rhodopseudomonas acidophila, Rhodopseudomonas palustris , or Rhodocyclus gelatinosus . These isolates exhibited degrees of atrazine resistance which ranged from 1.5 to about 4 times greater than that of cognate reference strains (American Type Culture Collection) tested. Furthermore, all of the reference strains tested were more intrinsically resistant to atrazine than was Rhodobacter sphaeroides . No unique plasmids which might encode for herbicide degradation or inactivation were found in these isolates. Resistance to the herbicide in these isolates was not the result of diminished binding of the herbicide to the L subunit of the bacterial reaction center. Differences in herbicide resistance among the various species of this group may be the result of compositional and chemical differences in the individual reaction centers. However, the increase in atrazine resistance for the isolates characterized in this study probably occurs by undefined mechanisms and not necessarily by changes in the binding of the herbicide to the L subunit of the photosynthetic reaction center.