The Cytochrome-cBinding Surface of Reaction Centers fromRhodobacter sphaeroides

George Feher: a pioneer in reaction center research

Our understanding of photosynthesis has been greatly advanced by the elucidation of the structure and function of the reaction center (RC), the membrane protein responsible for the initial light-induced charge separation in photosynthetic bacteria and green plants. Although today we know a great deal about the details of the primary processes in photosynthesis, little was known in the early days. George Feher made pioneering contributions to photosynthesis research in characterizing RCs from photosynthetic bacteria following the ground-breaking work of Lou Duysens and Rod Clayton (see articles in this issue by van Gorkom and Wraight). The work in his laboratory at the University of California, San Diego, started in the late 1960s and continued for over 30 years. He isolated a pure RC protein and used magnetic resonance spectroscopy to study the primary reactants. Following this pioneering work, Feher studied the detailed structure of the RC and the basic electron and proton transfer functions that it performs using a wide variety of biophysical and biochemical techniques. These studies, together with work from many other researchers, have led to our present detailed understanding of these proteins and their function in photosynthesis. The present article is a brief historical account of his pioneering contributions to photosynthesis research. A more detailed description of his work can be found in an earlier biographical paper (Feher in Photosynth Res 55:1-40, 1998a).

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.

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.

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.

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

In the photosynthetic bacterium Rhodobacter sphaeroides, a water soluble cytochrome c2 (cyt c2) is the electron donor to the reaction center (RC), the membrane-bound pigment-protein complex that is the site of the primary light-induced electron transfer. To determine the interactions important for docking and electron transfer within the transiently bound complex of the two proteins, RC and cyt c2 were co-crystallized in two monoclinic crystal forms. Cyt c2 reduces the photo-oxidized RC donor (D+), a bacteriochlorophyll dimer, in the co-crystals in approximately 0.9 micros, which is the same time as measured in solution. This provides strong evidence that the structure of the complex in the region of electron transfer is the same in the crystal and in solution. X-ray diffraction data were collected from co-crystals to a maximum resolution of 2.40 A and refined to an R-factor of 22% (R(free)=26%). The structure shows the cyt c2 to be positioned at the center of the periplasmic surface of the RC, with the heme edge located above the bacteriochlorophyll dimer. The distance between the closest atoms of the two cofactors is 8.4 A. The side-chain of Tyr L162 makes van der Waals contacts with both cofactors along the shortest intermolecular electron transfer pathway. The binding interface can be divided into two domains: (i) A short-range interaction domain that includes Tyr L162, and groups exhibiting non-polar interactions, hydrogen bonding, and a cation-pi interaction. This domain contributes to the strength and specificity of cyt c2 binding. (ii) A long-range, electrostatic interaction domain that contains solvated complementary charges on the RC and cyt c2. This domain, in addition to contributing to the binding, may help steer the unbound proteins toward the right conformation.

Double mutant studies identify electrostatic interactions that are important for docking cytochrome c2 onto the bacterial reaction center

Cytochrome c2 (cyt) is the mobile electron donor to the reaction center (RC) in photosynthetic bacteria. The electrostatic interactions involved in the dynamics of docking of cyt onto the RC were examined by double mutant studies of the rates of electron transfer between six modified Rhodobacter sphaeroides RCs in which negatively charged acid residues were replaced with Lys and five modified Rhodobacter capsulatus Cyt c2 molecules in which positively charged Lys residues were replaced with Glu. We measured the second-order rate constant, k2, for electron transfer from the reduced cyt to the oxidized primary donor on the RC, which reflects the energy of the transition state for the formation of the active electron transfer complex. Strong interactions were found between Lys C99 and Asp M184/Glu M95, and between Lys C54 and Asp L261/Asp L257. The interacting residues were found to be located close to each other in the recently determined crystal structure of the cyt-RC complex [Axelrod, H., et al. (2002) J. Mol. Biol. (in press)]. The interaction energies were approximately inversely proportional to the distances between charges. These results support earlier suggestions [Tetreault, M., et al. (2001) Biochemistry 40, 8452-8462] that the structure of the transition state in solution resembles the structure of the cyt-RC complex in the cocrystal and indicate that specific electrostatic interactions facilitate docking of the cyt onto the RC in a configuration optimized for both binding and electron transfer. The specific interaction between Asp M184 and Lys C99 may help to nucleate short-range hydrophobic contacts.

Interaction between cytochrome c2 and the photosynthetic reaction center from Rhodobacter sphaeroides: effects of charge-modifying mutations on binding and electron transfer

The electrostatic interactions governing binding and electron transfer from cytochrome c(2) (cyt c(2)) to the reaction center (RC) from the photosynthetic bacteria Rhodobacter sphaeroides were studied by using site-directed mutagenesis to change the charges of residues on the RC surface. Charge-reversing mutations (acid --> Lys) decreased the binding affinity for cyt c(2). Dissociation constants, K(D) (0.3--250 microM), were largest for mutations of Asp M184 and nearby acid residues, identifying the main region for electrostatic interaction with cyt c(2). The second-order rate constants, k(2) (1--17 x 10(8) M(-1) s(-1)), increased with increasing binding affinity (log k(2) vs log 1/K(D) had a slope of approximately 0.4), indicating a transition state structurally related to the final complex. In contrast, first-order electron transfer rates, k(e), for the bound cyt did not change significantly (<3-fold), indicating that electron tunneling pathways were unchanged by mutation. Charge-neutralizing mutations (acid --> amide) showed changes in binding free energies of approximately 1/2 the free energy changes due to the corresponding charge-reversing mutations, suggesting that the charges in the docked complex remain well solvated. Charge-enhancing mutations (amide --> acid) produced free energy changes of the same magnitude (but opposite sign) as changes due to the charge-neutralizing mutations in the same region, indicating a diffuse electrostatic potential due to cyt c(2). A two-domain model is proposed, consisting of an electrostatic docking domain with charged surfaces separated by a water layer and a hydrophobic tunneling domain with atomic contacts that provide an efficient pathway for electron transfer.

Preferential binding of equine ferricytochrome c to the bacterial photosynthetic reaction center from Rhodobacter sphaeroides

Redox titration of horse heart cytochrome c (cyt c), in the presence of varying concentrations of detergent-solubilized photosynthetic reaction center (RC) from Rhodobacter sphaeroides, revealed an RC concentration-dependent decrease in the measured cyt c midpoint potential that is indicative of a 3.6 +/- 0.2-fold stronger binding affinity of oxidized cytochrome to a single binding site. This effect was correlated with preferential binding in the functional complex by redox titration of the fraction of RCs exhibiting microsecond, first-order, special pair reduction by cytochrome. A binding affinity ratio of 3.1 +/- 0.4 was determined by this second technique, confirming the result. Redox titration of flash-induced intracomplex electron transfer also showed the association in the electron transfer-active complex to be strong, with a dissociation constant of 0.17 +/- 0.03 microM. The tight binding is associated with a slow off-rate which, in the case of the oxidized form, can influence the kinetics of P(+) reduction. The pitfalls of the common use of xenon flashlamps to photoexcite fast electron-transfer reactions are discussed with relation to the first electron transfer from primary to secondary RC quinone acceptors. The results shed some light on the diversity of kinetic behavior reported for the cytochrome to RC electron-transfer reaction.

Effects of temperature and deltaGo on electron transfer from cytochrome c2 to the photosynthetic reaction center of the purple bacterium Rhodobacter sphaeroides

The kinetics of electron transfer from cytochrome c2 to the primary donor (P) of the reaction center from the photosynthetic purple bacterium Rhodobacter sphaeroides have been investigated by time-resolved absorption spectroscopy. Rereduction of P+ induced by a laser pulse has been measured at temperatures from 300 K to 220 K in a series of specifically mutated reaction centers characterized by altered midpoint redox potentials of P+/P varying from 410 mV to 765 mV (as compared to 505 mV for wild type). Rate constants for first-order electron donation within preformed reaction center-cytochrome c2 complexes and for the bimolecular oxidation of free cytochrome c2 have been obtained by multiexponential deconvolution of the kinetics. At all temperatures the rate of the fastest intracomplex electron transfer increases by more than two orders of magnitude as the driving force -deltaGo is varied over a range of 350 meV. The temperature and deltaGo dependences of the rate constant fit the Marcus equation well. Global analysis yields a reorganization energy lambda = 0.96 +/- 0.07 eV and a set of electronic matrix elements, specific for each mutant, ranging from 1.2 10(-4) eV to 2.5 10(-4) eV. Analysis in terms of the Jortner equation indicates that the best fit is obtained in the classical limit and restricts the range of coupled vibrational modes to frequencies lower than approximately 200 cm(-1). An additional slower kinetic component of P+ reduction, attributed to electron transfer from cyt c2 docked in a nonoptimal configuration of the complex, displays a Marcus type dependence of the rate constant upon deltaGo, characterized by a similar value of lambda (0.8 +/- 0.1 eV) and by an average electronic matrix element smaller by more than one order of magnitude. In all of the mutants, as the temperature is decreased below 260 K, both intracomplex reactions are abruptly inhibited, their rate being negligible at 220 K. The free energy dependence of the second-order rate constant for oxidation of cyt c2 in solution suggests that the collisional reaction is partially diffusion controlled, reaching the diffusion limit at exothermicities between 150 and 250 meV over the temperature range investigated.

Anion binding to cytochrome c2: implications on protein-Ion interactions in class I cytochromes c

The binding of several inorganic and carboxylate anions to cytochrome c2 from Rhodopseudomonas palustris has been investigated by monitoring the salt-induced changes in the redox potential of the heme, using an interpretative model based on the extended Debye-Hückel equation. Most anions were found to interact specifically with the protein at one or multiple sites. Binding constants to the oxidized protein in the range 10(1)-10(2) m-1 were determined from the anion concentration dependence of the chemical shift of the isotropically shifted heme methyl resonances. For several anions the stoichiometry and strength of the binding to cytochrome c2 were found comparable with those determined for mitochondrial cytochromes c, in spite of the limited sequence similarity (less than 40%) and the lower positive charge of the bacterial protein. These analogies were interpreted as indicative of the existence of common binding sites which are proposed to be located in the conserved lysine-rich domain around the solvent-exposed heme edge, which is also the surface area likely involved in the interaction with redox partners. The changes in E degrees due to partial neutralization of the positive charge of cytochrome c2 due to specific anion binding were found comparable with those for the mitochondrial species.

Cross-linked electron transfer complex between cytochrome c2 and the photosynthetic reaction center of Rhodobacter sphaeroides

Electron donation from the soluble cytochrome (cyt) c2 to the photooxidized primary donor, P+, of reaction centers isolated from Rhodobacter sphaeroides was studied by using chemical zero-length cross-linking. This cross-linking stabilizes a 1:1 covalent complex between subunit M of the reaction center and cyt c2. In 80% of the reaction centers, P+ generated by a laser flash is reduced by covalently bound cyt c2. Kinetics of P+ reduction show (i) a fast phase with a half-life of 0.7 micros similar to that observed for electron transfer in the noncovalent proximal complex and (ii) a slow phase (t1/2 = 60 micros) that is attributed to a cyt c2 bound less favorably for electron transfer. Its relationship with similar kinetic phases attributed to a distal conformation of the complex in previous studies is discussed. Both kinetic phases are slightly accelerated upon addition of glycerol. Upon addition of reduced soluble cyt c2 to the cross-linked complex the kinetics of both phases are not affected. The kinetics of P+ reduction following the second flash (20 ms after the first) show that a complex is formed between soluble cyt c2 and the cross-linked complex, in which electron transfer takes place in the millisecond time domain. Cross-linked cyt c2 in complexes which give rise to the two kinetic phases of P+ reduction shows almost pH-independent midpoint redox potentials between pH 6 and 9.5. This behavior is at variance with that of free cyt c2, the midpoint potential of which is affected by at least two protonable groups within this pH range. The cross-linked RC-cyt c2 complex allowed study of the effects of temperature on the electron transfer reaction without a possible disturbance by dissociation of the complex. In the 250-300 K range, Arrhenius behavior is observed showing activation energies of 11.7 and 8.0 kJ/mol for the faster and the slower kinetic phases, respectively, which are remarkably lower than the activation energy of 20.5 kJ/mol for the fast P+ reduction by soluble cyt c2 [Venturoli, G., Mallardi, A., & Mathis, P. (1993) Biochemistry 32, 13245-13253]. Between 250 and 230 K, a fall-off in amplitude is observed for both kinetic phases indicating that intracomplex electron transfer is blocked at low temperatures.

Structure and function of cytochrome c2 in electron transfer complexes with the photosynthetic reaction center of Rhodobacter sphaeroides: optical linear dichroism and EPR

The photosynthetic reaction center (RC) and its secondary electron donor the water-soluble cytochrome (cyt) c2 from the purple bacterium Rhodobacter sphaeroides have been used in cross-linked and non-cross-linked complexes, oriented in compressed gels or partially dried multilayers, to study the respective orientation of the primary donor P (BChl dimer) and of cyt c2. Three methods were used: (i) Polarized optical absorption spectra at 295 and 10 K were measured and the linear dichroism of the two individual transitions (Qx, Qy), which are nearly degenerate within the alpha-band of reduced cyt c2, was determined. Attribution of the polarization directions to the molecular axes within the heme plane yielded the average cyt orientation in the complexes. (ii) Time-resolved flash absorption measurements using polarized light allowed determination of the orientation of cyt c2 in complexes which differ in their kinetics of electron transfer. (iii) EPR spectroscopy of ferricyt c2 in cross-linked RC-cyt c2 complexes was used to determine the angle between the heme and the membrane plane. The results suggest the following structural properties for the docking of cyt c2 to the RC: (i) In cross-linked complexes, the two cytochromes displaying half-lives of 0.7 and 60 micros for electron transfer to P+ are similarly oriented (difference < 10 degrees). (ii) For cross-linked cyt c2 the heme plane is parallel to the symmetry axis of the RC (0 degrees +/- 10 degrees). Moreover, the Qy transition, which is assumed to be polarized within the ring III-ring I direction of the heme plane, makes an angle of 56 degrees +/- 1 degree with the symmetry axis. (iii) The dichroism spectrum for the fast phase (0.7 micros) for the non-cross-linked cyt c2-RC complex suggests an orientation similar to that of cross-linked cyt c2, but the heme plane is tilted about 20 degrees closer to the membrane. An alternative model is that two or more bound states of cyt c2 with heme plane tilt angles between 0 degrees and 30 degrees allow the fast electron transfer. Zero-length cross-linking of cyt c2 may take place in one of these bound states. These orientations of cyt c2 are compared to different structural models of RC-cyt c2 complexes proposed previously. The relation of the two kinetic phases observed in cross-linked cyt c2 complexes to biphasic kinetics of the mobile reaction partners is discussed with respect to the dynamic electrostatic interactions during the formation of a docking complex and its dissociation. A mechanism is proposed in which a pre-orientation of cyt c2 relative to the membrane plane occurs by interaction of its strong electrostatic dipole with the negative surface charges of the RC. The optimal matching of the oppositely charged surfaces of the two proteins necessitates further rotation of the cyt around its dipole axis.

Co-crystallization and characterization of the photosynthetic reaction center-cytochrome c2 complex from Rhodobacter sphaeroides

The photosynthetic reaction center (RC) of Rhodobacter sphaeroides and cytochrome c2 (cyt c2), its physiological secondary electron donor, have been co-crystallized. The molar ratio of RC/cyt c2 was found by SDS-PAGE and optical absorbance changes in the co-crystals to be 4. The crystals diffracted X-rays to 3.5 angstroms. However, the resolution degraded during data collection. A data set, 82.5% complete, was collected to 4.5 angstroms. The crystals belong to the tetragonal space group P4(3)2(1)2, with unit cell dimensions of a = b = 142.7 angstroms and c = 254.8 angstroms. The positions of the RCs in the unit cell were determined by molecular replacement. A comparable search for the cyt c2 by this method was unsuccessful because of the small contribution of the cytochrome to the total scattering and because of its low occupancy. The cyt c2 was positioned manually into patches of difference electron density, adjacent to the periplasmic surface of the M polypeptide subunit of the RC. The difference electron density was not sufficient for precise positioning of the cyt c2, and its orientation was modeled by placing the exposed edge of the heme toward the primary donor of the reaction center D and by forming pairs for electrostatically interacting RC and cyt c2 amino acid residues. The RC-cyt c2 structure derived from the co-crystal data was supported by use of omit maps and structure refinement analyses. Cyt c2 reduces the photooxidized primary donor D+ in 0.9 +/- 0.1 micros in the co-crystals, which is the same as the fast electron transfer rate in vivo and in solution. This result provides strong evidence that the structure of the complex in the co-crystal is the same as in solution. Two additional methods were used to investigate the structure of the RC-cyt c2 complex: (i) Docking calculations based on interprotein electrostatic interactions identified possible binding positions of the cyt c2 on the RC. The cyt c2 position with the lowest electrostatic energy is very similar to that of the cyt c2 in the proposed co-crystal structure. (ii) Site-directed mutagenesis was used to modify two aspartic acid residues (M184 and L155) on the periplasmic surface of the RC. Cyt c2 binding affinity to these RCs and electron transfer rates to D+ in these RCs support the co-crystal structure of th RC-cyt c2 complex.

Relationship between the oxidation potential of the bacteriochlorophyll dimer and electron transfer in photosynthetic reaction centers

The primary electron donor in the photosynthetic reaction center from purple bacteria is a bacteriochlorophyll dimer containing four conjugated carbonyl groups that may form hydrogen bonds with amino acid residues. Spectroscopic analyses of a set of mutant reaction centers confirm that hydrogen bonds can be formed between each of these carbonyl groups and histidine residues in the reaction center subunits. The addition of each hydrogen bond is correlated with an increase in the oxidation potential of the dimer, resulting in a 355-mV range in the midpoint potential. The resulting changes in the free-energy differences for several reactions involving the dimer are related to the electron transfer rates using the Marcus theory. These reactions include electron transfer from cytochrome c2 to the oxidized dimer, charge recombination from the primary electron acceptor quinone, and the initial forward electron transfer.

Protein interaction sites obtained via sequence homology. The site of complexation of electron transfer partners of cytochrome c revealed by mapping amino acid substitutions onto three-dimensional protein surfaces

Amino acid substitutions in all but the most divergent of cytochromes c have been categorized as being conservative or radical and mapped onto the three-dimensional structure of yeast cytochrome c. Color-coded, space-filling representations reveal a large 24 A diameter surface area which is invariant or conservatively substituted on the front left face of the cytochrome c molecule. Chemical modifications and mutations which inhibit complex formation and electron transfer with reaction partners also map to this surface. In sharp contrast, the back side of the protein is randomly substituted with both conservative and radical replacements. The invariant/conservatively substituted surface on the front of cytochrome c thus defines the site of interaction with redox partners and provides a measure of its dimensions. Further, this analysis strongly suggests that there is only a single site of oxidation and reduction on cytochrome c for all of its physiological reactions. The same analysis applied to bacterial cytochrome c2 shows that its conserved surface is similar in size and location to that of cytochrome c. Analyses of native and model reaction partners of cytochromes c and c2, such as cytochrome b5, plastocyanin, and bacterial photosynthetic reaction centers, also reveal probable active site surfaces for complexation and electron transfer, which are complementary in size to that of the c-type cytochromes. The availability of a three-dimensional structure and of several closely related amino acid sequences for a given functional class of protein is the only limitation on this type of analysis, which can then serve as a basis for designing site-directed mutagenesis experiments.

The reaction center associated tetraheme cytochrome subunit from Chromatium vinosum revisited: a reexamination of its EPR properties

The heme components of chromatophore membranes from the purple bacterium Chromatium vinosum have been studied by EPR. Five different heme species could be distinguished on the basis of their g values, redox midpoint potentials, and orientations of heme planes with respect to the membrane plane: gz = 2.94, Em = +10 mV, 40 degrees-50 degrees; gz = 2.94, Em = +10 mV, 0 degree; gz = 3.1, Em = +330 mV, 90 degrees; gz = 3.3, Em = 360 mV, 30 degrees; gz = 3.4, Em = 0 mV, no detectable orientation. Four of these five hemes (gz = 3.3, gz = 3.1, and 2x gz = 2.94) were ascribed to the tetraheme cytochrome subunit associated with the photosynthetic reaction center of this bacterium. Some of the results obtained have already been reported previously [Tiede, D.M., Leigh, J.S., & Dutton, P.L. (1978) Biochim. Biophys. Acta 503, 524-544] and have led to a model for the tetraheme cytochrome subunit in Chromatium which is significantly different from the three-dimensional structure of the reaction center associated subunit in the purple bacterium Rhodopseudomonas viridis. The additional data obtained in our work, however, require a reinterpretation of the previously published results. The model arrived at is in general agreement with the X-ray structure from Rhodopseudomonas viridis. A model rationalizing the detailed differences between the structure of the Rhodopseudomonas viridis cytochrome subunit and the data obtained on tetraheme subunits from other photosynthetic bacteria is presented.

Electron-transfer kinetics and electrostatic properties of the Rhodobacter sphaeroides reaction center and soluble c-cytochromes

The kinetics of electron transfer between the Rhodobacter sphaeroides R-26 reaction center and nine soluble c-cytochromes have been analyzed and compared to the patterns of the surface electrostatic potentials for each of the proteins. Characteristic first-order electron-transfer rates for 1:1 complexes formed at low ionic strength between the reaction center and the different c-cytochromes were identified and found to vary by a factor of almost 100, while second-order rates were found to differ by greater than 10(6). A correlation was found between the location of likely electrostatic interaction domains on each cytochrome and its characteristic rate of electron transfer. The interaction domains were identified by mapping electrostatic potentials, calculated from the Poisson-Boltzmann equation, onto simulated "encounter surfaces" for each of the cytochromes and the reaction center. For the reaction center, the c-cytochrome binding domain was found to have almost exclusively net negative potential (< -3 kT) and to be shifted slightly toward the M-subunit side of the reaction center. The location of interaction domains of complementary, positive potential (> 3 kT) differed for each cytochrome. The correspondence between electrostatic, structural, and kinetic properties of 1:1 reaction center-cytochrome complexes leads to a proposed mechanism for formation of reaction center-cytochrome electron-transfer complexes that is primarily driven by the juxtaposition of regions of delocalized complementary potential. In this mechanism the clustering of charged residues is of primary importance and not the location of specific residues. A consequence of this mechanism is that many different sets of charge distributions are predicted to be capable of stabilizing a specific configuration for a reaction center-cytochrome complex. This mechanism for reaction center association with water-soluble c-cytochromes fits molecular recognition mechanisms proposed for c-cytochromes in nonphotosynthetic systems. In general, the kinetic scheme for reaction center driven cytochrome oxidation was found to vary between a simple two-state model, involving cytochrome in free and reaction center bound states, and a three-state model, that includes cytochrome binding in kinetically competent ("proximal") and incompetent ("distal") modes. The kinetically incompetent mode of cytochrome binding is suggested not to be an intrinsic feature of the reaction center-cytochrome association but is likely to be due to variation in the physical state of the reaction center.