X-ray structure determination of the cytochrome c2: reaction center electron transfer complex from Rhodobacter sphaeroides

Transition state and encounter complex for fast association of cytochrome c2 with bacterial reaction center

Electrostatic interactions strongly enhance the electron transfer reaction between cytochrome (Cyt) c(2) and reaction center (RC) from photosynthetic bacteria, yielding a second-order rate constant, k(2) approximately 10(9) s(-1).M(-1), close to the diffusion limit. The proposed mechanism involves an encounter complex (EC) stabilized by electrostatic interactions, followed by a transition state (TS), leading to the bound complex active in electron transfer. The effect of electrostatic interactions was previously studied by Tetreault et al. [Tetreault, M., Cusanovich, M., Meyer, T., Axelrod, H. & Okamura, M. Y. (2002) Biochemistry 41, 5807-5815] by measuring k(2) for RC and Cyt molecules with modified charged residues at the binding interface. The present work is a computational analysis of this kinetic study to determine the ensemble of configurations of the TS and EC. Changes in the TS energies due to different mutations were compared with differences in the calculated electrostatic energies for a wide range of Cyt/RC configurations. The TS ensemble, obtained from structures having the highest correlation coefficients in the comparison with experimental data, has the Cyt displaced by approximately 10 A from its position in x-ray crystal structure, close to the average position of the EC ensemble, with strong electrostatic interactions between Cyt on the M subunit side of the RC surface. The heme of the Cyt is oriented toward Tyr L162 on the RC, the tunneling contact in the bound final state on the RC. The similarity between the structures of the EC, TS, and bound state can account for the rapid rate of association responsible for fast diffusion-controlled electron transfer.

Classical force field parameters for the heme prosthetic group of cytochrome c

Accurate force fields are essential for describing biological systems in a molecular dynamics simulation. To analyze the docking of the small redox protein cytochrome c (cyt c) requires simulation parameters for the heme in both the reduced and oxidized states. This work presents parameters for the partial charges and geometries for the heme in both redox states with ligands appropriate to cyt c. The parameters are based on both protein X-ray structures and ab initio density functional theory (DFT) geometry optimizations at the B3LYP/6-31G* level. The simulations with the new parameter set reproduce the geometries of the X-ray structures and the interaction energies between water and heme prosthetic group obtained from B3LYP/6-31G* calculations. The parameter set developed here will provide new insights into docking processes of heme containing redox proteins.

Two distinct binding sites for high potential iron-sulfur protein and cytochrome c on the reaction center-bound cytochrome of Rubrivivax gelatinosus

The photosynthetic cyclic electron transfer of the purple bacterium Rubrivivax gelatinosus, involving the cytochrome bc(1) complex and the reaction center, can be carried out via two pathways. A high potential iron-sulfur protein (HiPIP) acts as the in vivo periplasmic electron donor to the reaction center (RC)-bound cytochrome when cells are grown under anaerobic conditions in the light, while cytochrome c is the soluble electron carrier for cells grown under (8)aerobic conditions in the dark. A spontaneous reversion of R. gelatinosus C244, a defective mutant in synthesis of the RC-bound cytochrome by insertion of a Km(r) cassette leading to gene disruption with a slow growth rate, restores the normal photosynthetic growth. This revertant, designated C244-P1, lost the Km(r) cassette but synthesized a RC-bound cytochrome with an external 77-amino acid insertion derived from the cassette. We characterized the RC-bound cytochrome of this mutant by EPR, time-resolved optical spectroscopy, and structural analysis. We also investigated the in vivo electron transfer rates between the two soluble electron donors and this RC-bound cytochrome. Our results demonstrated that the C244-P1 RC-bound cytochrome is still able to receive electrons from HiPIP, but it is no longer reducible by cytochrome c(8). Combining these experimental and theoretical protein-protein docking results, we conclude that cytochrome c(8) and HiPIP bind the RC-bound cytochrome at two distinct but partially overlapping sites.

Orientated binding of photosynthetic reaction centers on gold using NiNTA self-assembled monolayers

Coupling of photosynthetic reaction centers (RCs) with inorganic surfaces is attractive for the identification of the mechanisms of interprotein electron transfer (ET) and for possible applications in construction of photo- and chemosensors. Here we show that RCs from Rhodobacter sphaeroides can be immobilized on gold surfaces with the RC primary donor looking towards the substrate by using a genetically engineered poly-histidine tag (His(7)) at the C-terminal end of the M-subunit and a Ni-NTA terminated self-assembled monolayer (SAM). In the presence of an electron acceptor, ubiquinone-10, illumination of this RC electrode generates a cathodic photocurrent. The action spectrum of the photocurrent coincides with the absorption spectrum of RC and the photocurrent decreases in response to the herbicide, atrazine, confirming that the RC is the primary source of the photoresponse. Disruption of the Ni-NTA-RC bond by imidazole leads to about 80% reduction of the photocurrent indicating that most of the photoactive protein is specifically bound to the electrode through the linker.

A Brownian dynamics study: the effect of a membrane environment on an electron transfer system

During the past few years, three-dimensional crystal structures of many of the important integral membrane proteins responsible for the bioenergetic processes of photosynthesis and respiration have been determined. Moreover, a few crystal structures of protein-protein complexes have become available that characterize the interaction between those membrane proteins and the electron carrier protein cytochrome c. Here, we address the association kinetics for binding of cytochrome c to cytochrome c oxidase (COX) from Paracoccus denitrificans by Brownian dynamics simulations. The effects of ionic strength and protein mutations were studied for two different cytochrome c species: the positively charged, dipolar horse heart cytochrome c and the negatively charged physiological electron transfer partner cytochrome c(552). We studied association toward "naked" COX and toward membrane-embedded COX where the membrane is represented as an uncharged DPPC bilayer modeled in atomistic detail. For the nonnatural association toward "naked" COX, the association rates are >100 times larger for horse heart cytochrome c than for cytochrome c(552). Interestingly, the presence of the lipid bilayer leads to a dramatic decrease of the association rate of horse heart cytochrome c, but slightly enhances association of cytochrome c(552), leading to very similar association rates of both proteins to membrane-embedded COX. This finding from computational modeling studies may reflect the optimization of surface patches and of the total net charge on electron transfer pairs in nature.

Interactions between cytochrome c2 and photosynthetic reaction center from Rhodobacter sphaeroides: changes in binding affinity and electron transfer rate due to mutation of interfacial hydrophobic residues are strongly correlated

The structure of the complex between cytochrome c(2) (cyt) and the photosynthetic reaction center (RC) from Rhodobacter sphaeroides shows contacts between hydrophobic residues Tyr L162, Leu M191, and Val M192 on the RC and the surface of the cyt [Axelrod et al. (2002) J. Mol. Biol. 319, 501-515]. The role of these hydrophobic residues in binding and electron transfer was investigated by replacing them with Ala and other residues. Mutations of the hydrophobic residues generally resulted in relatively small changes in the second-order electron-transfer rate k(2) (Brönsted coefficient, alpha( )()= 0.15 +/- 0.05) indicating that the transition state for association occurs before short-range hydrophobic contacts are established. Larger changes in k(2), found in some cases, were attributed to a change in the second-order mechanism from a diffusion controlled regime to a rapidly reversible binding regime. The association constant, K(A), of the cyt and the rate of electron transfer from the bound cyt, k(e), were both decreased by mutation. Replacement of Tyr L162, Leu M191, or Val M192 by Ala decreased K(A) and k(e) by factors of 130, 10, 0.6, and 120, 9, 0.6, respectively. The largest changes were obtained by mutation of Tyr L162, showing that this residue plays a key role in both binding and electron transfer. The binding affinity, K(A), and electron-transfer rate, k(e) were strongly correlated, showing that changes of hydrophobic residues affect both binding and electron transfer. This correlation suggests that changes in distance across hydrophobic interprotein contacts have similar effects on both electron tunneling and binding interactions.

Interaction of cytochrome c with cytochrome oxidase: two different docking scenarios

Cytochrome c is the specific and efficient electron transfer mediator between the two last redox complexes of the mitochondrial respiratory chain. Its interaction with both partner proteins, namely cytochrome c(1) (of complex III) and the hydrophilic Cu(A) domain (of subunit II of oxidase), is transient, and known to be guided mainly by electrostatic interactions, with a set of acidic residues on the presumed docking site on the Cu(A) domain surface and a complementary region of opposite charges exposed on cytochrome c. Information from recent structure determinations of oxidases from both mitochondria and bacteria, site-directed mutagenesis approaches, kinetic data obtained from the analysis of isolated soluble modules of interacting redox partners, and computational approaches have yielded new insights into the docking and electron transfer mechanisms. Here, we summarize and discuss recent results obtained from bacterial cytochrome c oxidases from both Paracoccus denitrificans, in which the primary electrostatic encounter most closely matches the mitochondrial situation, and the Thermus thermophilus ba(3) oxidase in which docking and electron transfer is predominantly based on hydrophobic interactions.

The architecture of the binding site in redox protein complexes: Implications for fast dissociation

Interprotein electron transfer is characterized by protein interactions on the millisecond time scale. Such transient encounters are ensured by extremely high rates of complex dissociation. Computational analysis of the available crystal structures of redox protein complexes reveals features of the binding site that favor fast dissociation. In particular, the complex interface is shown to have low geometric complementarity and poor packing. These features are consistent with the necessity for fast dissociation since the absence of close packing facilitates solvation of the interface and disruption of the complex.

Electron transfer from HiPIP to the photooxidized tetraheme cytochrome subunit of Allochromatium vinosum reaction center: new insights from site-directed mutagenesis and computational studies

The kinetics of electron transfer from reduced high-potential iron-sulfur protein (HiPIP) to the photooxidized tetraheme cytochrome c subunit (THC) bound to the photosynthetic reaction center (RC) from the purple sulfur bacterium Allochromatium vinosum were studied under controlled redox conditions by flash absorption spectroscopy. At ambient redox potential Eh = +200 mV, where only the high-potential (HP) hemes of the THC are reduced, the electron transfer from HiPIP to photooxidized HP heme(s) follows second-order kinetics with rate constant k = (4.2 +/- 0.2) 10(5) M(-1) s(-1) at low ionic strength. Upon increasing the ionic strength, k increases by a maximum factor of ca. 2 at 640 mM KCl. The role of Phe48, which lies on the external surface of HiPIP close to the [Fe4S4] cluster and presumably on the electron transfer pathway to cytochrome heme(s), was investigated by site-directed mutagenesis. Substitution of Phe48 with arginine, aspartate, and histidine completely prevents electron donation. Conversely, electron transfer is still observed upon substitution of Phe48 with tyrosine and tryptophan, although the rate is decreased by more than 1 order of magnitude. These results suggest that Phe48 is located on a key protein surface patch essential for efficient electron transfer, and that the presence of an aromatic hydrophobic residue on the putative electron-transfer pathway plays a critical role. This conclusion was supported by protein docking calculations, resulting in a structural model for the HiPIP-THC complex, which involves a docking site close to the LP heme farthest from the bacteriochlorophyll special pair.

Structure and function of photosystem I: interaction with its soluble electron carriers and external antenna systems

Photosystem I (PS I) is a large membrane protein complex that catalyzes the first step of solar conversion, the light-induced transmembrane electron transfer, and generates reductants for CO2 assimilation. It consists of 12 different proteins and 127 cofactors that perform light capturing and electron transfer. The function of PS I includes inter-protein electron transfer between PS I and smaller soluble electron transfer proteins. The structure of PS I is discussed with respect to the potential docking sites for the soluble electron acceptors, ferredoxin/flavodoxin, at the stromal side and the soluble electron donors, cytochrome c6/plastocyanin, at the luminal side of the PS I complex. Furthermore, the potential interaction sites with the peripheral antenna proteins are discussed.

Structural and redox plasticity in the heterodimeric periplasmic nitrate reductase

The structure of the respiratory nitrate reductase (NapAB) from Rhodobacter sphaeroides, the periplasmic heterodimeric enzyme responsible for the first step in the denitrification process, has been determined at a resolution of 3.2 A. The di-heme electron transfer small subunit NapB binds to the large subunit with heme II in close proximity to the [4Fe-4S] cluster of NapA. A total of 57 residues at the N- and C-terminal extremities of NapB adopt an extended conformation, embracing the NapA subunit and largely contributing to the total area of 5,900 A(2) buried in the complex. Complex formation was studied further by measuring the variation of the redox potentials of all the cofactors upon binding. The marked effects observed are interpreted in light of the three-dimensional structure and depict a plasticity that contributes to an efficient electron transfer in the complex from the heme I of NapB to the molybdenum catalytic site of NapA.

Continuum Electrostatic Model for the Binding of Cytochrome c2 to the Photosynthetic Reaction Center from Rhodobacter sphaeroides

Electrostatic interactions are important for protein-protein association. In this study, we examined the electrostatic interactions between two proteins, cytochrome c(2) (cyt c(2)) and the reaction center (RC) from the photosynthetic bacterium Rhodobacter sphaeroides, that function in intermolecular electron transfer in photosynthesis. Electrostatic contributions to the binding energy for the cyt c(2)-RC complex were calculated using continuum electrostatic methods based on the recent cocrystal structure [Axelrod, H. L., et al. (2002) J. Mol. Biol. 319, 501-515]. Calculated changes in binding energy due to mutations of charged interface residues agreed with experimental results for a protein dielectric constant epsilon(in) of 10. However, the electrostatic contribution to the binding energy for the complex was close to zero due to unfavorable desolvation energies that compensate for the favorable Coulomb attraction. The electrostatic energy calculated as a function of displacement of the cyt c(2) from the bound position showed a shallow minimum at a position near but displaced from the cocrystal configuration. These results show that although electrostatic steering is present, other short-range interactions must be present to contribute to the binding energy and to determine the structure of the complex. Calculations made to model the experimental data on association rates indicate a solvent-separated transition state for binding in which the cyt c(2) is displaced approximately 8 A above its position in the bound complex. These results are consistent with a two-step model for protein association: electrostatic docking of the cyt c(2) followed by desolvation to form short-range van der Waals contacts for rapid electron transfer.

Lipidic cubic phase crystal structure of the photosynthetic reaction centre from Rhodobacter sphaeroides at 2.35A resolution

Well-ordered crystals of the bacterial photosynthetic reaction centre from Rhodobacter sphaeroides were grown from a lipidic cubic phase. Here, we report the type I crystal packing that results from this crystallisation medium, for which 3D crystals grow as stacked 2D crystals, and the reaction centre X-ray structure is refined to 2.35A resolution. In this crystal form, the location of the membrane bilayer could be assigned with confidence. A cardiolipin-binding site is found at the protein-protein interface within the membrane-spanning region, shedding light on the formation of crystal contacts within the membrane. A chloride-binding site was identified in the membrane-spanning region, which suggests a putative site for interaction with the light-harvesting complex I, the cytochrome bc(1) complex or PufX. Comparisons with the X-ray structures of this reaction centre deriving from detergent-based crystals are drawn, indicating that a slight compression occurs in this lipid-rich environment.

Design of a ruthenium-labeled cytochrome c derivative to study electron transfer with the cytochrome bc1 complex

A new ruthenium-cytochrome c derivative was designed to study electron transfer from cytochrome bc1 to cytochrome c (Cc). The single sulfhydryl on yeast H39C;C102T iso-1-Cc was labeled with Ru(2,2'-bipyrazine)2(4-bromomethyl-4'-methyl-2,2'-bipyridine) to form Ru(z)-39-Cc. The Ru(z)-39-Cc derivative has the same steady-state activity with yeast cytochrome bc1 as wild-type yeast iso-1-Cc, indicating that the ruthenium complex does not interfere in the binding interaction. Laser excitation of reduced Ru(z)-39-Cc results in electron transfer from heme c to the excited state of ruthenium with a rate constant of 1.5 x 10(6) x s(-1). The resulting Ru(I) is rapidly oxidized by atmospheric oxygen in the buffer. The yield of photooxidized heme c is 20% in a single flash. Flash photolysis of a 1:1 complex between reduced yeast cytochrome bc1 and Ru(z)-39-Cc at low ionic strength leads to rapid photooxidation of heme c, followed by intracomplex electron transfer from cytochrome c1 to heme c with a rate constant of 1.4 x 10(4) x s(-1). As the ionic strength is raised above 100 mM, the intracomplex phase disappears, and a new phase appears due to the bimolecular reaction between solution Ru-39-Cc and cytochrome bc1. The interaction of yeast Ru-39-Cc with yeast cytochrome bc1 is stronger than that of horse Ru-39-Cc with bovine cytochrome bc1, suggesting that nonpolar interactions are stronger in the yeast system.

Characterization of the interaction of Rhodobacter capsulatus cytochrome c peroxidase with charge reversal mutants of cytochrome c(2)

Steady-state kinetics for the reaction of Rhodobacter capsulatus bacterial cytochrome c peroxidase (BCCP) with its substrate cytochrome c(2) were investigated. The Rb. capsulatus BCCP is dependent on calcium for activation as previously shown for the Pseudomonas aeruginosa BCCP and Paracoccus denitrificans enzymes. Furthermore, the activity shows a bell-shaped pH dependence with optimum at pH 7.0. Enzyme activity is greatest at low ionic strength and drops off steeply as ionic strength increases, resulting in an apparent interaction domain charge product of -13. All cytochromes c(2) show an asymmetric distribution of surface charge, with a concentration of 14 positive charges near the exposed heme edge of Rb. capsulatus c(2) which potentially may interact with approximately 6 negative charges, localized near the edge of the high-potential heme of the Rb. capsulatus BCCP. To test this proposal, we constructed charge reversal mutants of the 14 positively charged residues located on the front face of Rb. capsulatus cytochrome c(2) and examined their effect on steady-state kinetics with BCCP. Mutated residues in Rb. capsulatus cytochrome c(2) that showed the greatest effects on binding and enzyme activity are K12E, K14E, K54E, K84E, K93E, and K99E, which is consistent with the site of electron transfer being located at the heme edge. We conclude that a combination of long-range, nonspecific electrostatic interactions as well as localized salt bridges between, e.g., cytochrome c(2) K12, K14, K54, and K99 with BCCP D194, D241, and D6, account for the observed kinetics.

Protein-lipid interactions in the purple bacterial reaction centre

The purple bacterial reaction centre uses the energy of sunlight to power energy-requiring reactions such as the synthesis of ATP. During the last 20 years, a combination of X-ray crystallography, spectroscopy and mutagenesis has provided a detailed insight into the mechanism of light energy transduction in the bacterial reaction centre. In recent years, structural techniques including X-ray crystallography and neutron scattering have also been used to examine the environment of the reaction centre. This mini-review focuses on recent studies of the surface of the reaction centre, and briefly discusses the importance of the specific protein-lipid interactions that have been resolved for integral membrane proteins.