Energetics of proton transfer pathways in reaction centers from Rhodobacter sphaeroides. The Glu-H173 activated mutants

Electron transfer between the primary and secondary quinones (Q(A), Q(B)) in the bacterial photosynthetic reaction center (bRC) is coupled with proton uptake at Q(B). The protons are conducted from the cytoplasmic side, probably with the participation of two water channels. Mutations of titratable residues like Asp-L213 to Asn (inhibited mutant) or the double mutant Glu-L212 to Ala/Asp-L213 to Ala inhibit these electron transfer-coupled proton uptake events. The inhibition of the proton transfer (PT) process in the single mutant can be restored by a second mutation of Arg-M233 to Cys or Arg-H177 to His (revertant mutant). These revertant mutants shed light on the location of the main proton transfer pathway of wild type bRC. In contrast to the wild type and inhibited mutant bRC, the revertant mutant bRC showed notable proton uptake at Glu-H173 upon formation of the Q(B)- state. In all of these mutants, the pK(a) of Asp-M17 decreased by 1.4-2.4 units with respect to the wild type bRC, whereas a significant pK(a) upshift of up to 5.8 units was observed at Glu-H122, Asp-H170, Glu-H173, and Glu-H230 in the revertant mutants. These residues belonging to the main PT pathway are arranged along water channel P1 localized mainly in subunit H. bRC possesses subunit H, which has no counterpart in photosystem II. Thus, bRC may possess alternative PT pathways involving water channels in subunit H, which becomes active in case the main PT pathway is blocked.     

Comparison of proton transfer paths to the QA and QB sites of the Rb. sphaeroides photosynthetic reaction centers

Photosynthesis Research - The photosynthetic bacterial reaction centers from purple non-sulfur bacteria use light energy to drive the transfer of electrons from cytochrome c to ubiquinone....     

Identification of proton transfer pathways in the X-ray crystal structure of the bacterial reaction center from Rhodobacter sphaeroides

Structural features that have important implications for the fundamental process of transmembrane proton transfer are examined in the recently published high resolution atomic structures of the reaction center (RC) from Rhodobacter sphaeroides in the dark adapted state (DQ_AQ_B) and the charged separated state (D⁺Q_AQ_B ^–); the latter is the active state for proton transfer to the semiquinone. The structures have been determined at 2.2 Å and 2.6 Å resolution, respectively, as reported by Stowell et al. (1997) [Science 276: 812–816]. Three possible proton transfer pathways (P1, P2, P3) consisting of water molecules and/or protonatable residues were identified which connect the Q_B binding region with the cytoplasmic exposed surface at Asp H224 & Asp M240 (P1), Tyr M3 (P2) and Asp M17 (P3). All three represent possible pathways for proton transfer into the RC. P1 contains an uninterrupted chain of water molecules. This path could, in addition, facilitate the exchange of quinone for quinol during the photocycle by allowing water to move into and out of the binding pocket. Located near these pathways is a cluster of electrostatically interacting acid residues (Asp-L213, Glu-H173, Asp-M17, Asp H124, Asp-L210 and Asp H170) each being within 4.5 Å of a neighboring carboxylic acid or a bridging water molecule. This cluster could serve as an internal proton reservoir facilitating fast protonation of Q_B ^– that could occur at a rate greater than that attainable by proton uptake from solution.     

Protein fluorescence of photosynthetic reaction centers from Rhodopseudomonas sphaeroides

Luminescence emitted by tryptophan residues of reaction center (RC) preparations was studied. The RG preparations were isolated from the photosynthetic bacterium Rhodopseudomonas sphaeroides by treatment with lauryl dimethyl amine oxide (LDAO). After excitation at lambda 280 nm the quantum yield of luminescence is 0,02. It is shown that 60% of tryptophanyls are located inside the protein globule in the surrounding of relaxating polar groups and the rest approximately 40% on the outer surface of the globule--predominantly in the positively charged region of the LDAO-RC protein--in the surrounding of protein-bound water molecules. There is a correlation between the pH dependencies of the position of the peak of luminescence from tryptophanyls and effectivity of electron transfer from the primary (quinone) to secondary acceptor. The two parameters are invariant at pH from 7 to 9 and vary at pH less than 7 and pH greater than 9. The phenomena responsible for the observed correlation are discussed on the basis of pH-dependent changes in the RC protein which govern electron transport activity at the reaction center.     

Energetics of quinone-dependent electron and proton transfers in Rhodobacter sphaeroides photosynthetic reaction centers

Proteins bind redox cofactors, modifying their electrochemistry and affinity by specific interactions of the binding site with each cofactor redox state. Photosynthetic reaction centers from Rhodobacter sphaeroides have three ubiquinone-binding sites, Q(A), and proximal and distal Q(B) sites. Ubiquinones, which can be doubly reduced and bind 2 protons, have 9 redox states. However, only Q and Q(-) are seen in the Q(A) site and Q, Q(-), and QH(2) in the proximal Q(B) site. The distal Q(B) function is uncertain. Multiple conformation continuum electrostatics (MCCE) was used to compare the ubiquinone electrochemical midpoints (E(m)) and pK(a) values at these three sites. At pH 7, the Q(A)/Q(A)(-) E(m) is -40 mV and proximal Q(B)/Q(B)(-) -10 mV in agreement with the experimental values (assuming a solution ubiquinone E(m) of -145 mV). Q(B) reduction requires changes in nearby residue protonation and SerL223 reorientation. The distal Q(B)/Q(B)(-) E(m) is a much more unfavorable -260 mV. Q(A) and proximal Q(B) sites generally stabilize species with a -1 charge, while the distal Q(B) site prefers binding neutral species. In each site, the dianion is destabilized because favorable interactions with the residues and backbone increase with charge (q), while the unfavorable loss of solvation energy increases with q(2). Therefore, proton binding before a second reduction, forming QH and then QH(-), is always preferred to forming the dianion (Q(-)(2)). The final product QH(2) is higher in energy at the proximal Q(B) site than in solution; therefore, it binds poorly, favoring release. In contrast, QH(2) binds more tightly than Q at the distal Q(B) site.     

Nanosecond fluorescence from isolated photosynthetic reaction centers of Rhodopseudomonas sphaeroides

The time-course of fluorescence from reaction centers isolated from Rhodopseudomonas sphaeroides was measured using single-photon counting techniques. When electron transfer is blocked by the reduction of the electron-accepting quinones, reaction centers exhibit a relatively long-lived (delayed) fluorescence due to back reactions that regenerate the excited state (P*) from the transient radical-pair state, PF. The delayed fluorescence can be resolved into three components, with lifetimes of 0.7, 3.2 and 11 ns at 295 K. The slowest component decays with the same time-constant as the absorbance changes due to PF, and it depends on both temperature and magnetic fields in the same way that the absorbance changes do. The time-constants for the two faster components of delayed fluorescence are essentially independent of temperature and magnetic fields. The fluorescence also includes a very fast (prompt) component that is similar in amplitude to that obtained from unreduced reaction centers. The prompt fluorescence presumably is emitted mainly during the period before the initial charge-transfer reaction creates PF from P*. From the amplitudes of the prompt and delayed fluorescence, we calculate an initial standard free-energy difference between P* and PF of about 0.16 eV at 295 K, and 0.05 eV at 80 K, depending somewhat on the properties of the solvent. The multiphasic decay of the delayed fluorescence is interpreted in terms of relaxations in the free energy of PF with time, totalling about 0.05 eV at 295 K, possibly resulting from nuclear movements in the electron-carriers or the protein.     

Calculated protein and proton motions coupled to electron transfer: electron transfer from QA- to QB in bacterial photosynthetic reaction centers.

Reaction centers from Rhodobacter sphaeroides were subjected to Monte Carlo sampling to determine the Boltzmann distribution of side-chain ionization states and positions and buried water orientation and site occupancy. Changing the oxidation states of the bacteriochlorophyll dimer electron donor (P) and primary (QA) and secondary (QB) quinone electron acceptors allows preparation of the ground (all neutral), P+QA-, P+QB-, P0QA-, and P0QB- states. The calculated proton binding going from ground to other oxidation states and the free energy of electron transfer from QA-QB to form QAQB- (DeltaGAB) compare well with experiment from pH 5 to pH 11. At pH 7 DeltaGAB is measured as -65 meV and calculated to be -80 meV. With fixed protein positions as in standard electrostatic calculations, DeltaGAB is +170 meV. At pH 7 approximately 0.2 H+/protein is bound on QA reduction. On electron transfer to QB there is little additional proton uptake, but shifts in side chain protonation and position occur throughout the protein. Waters in channels leading from QB to the surface change site occupancy and orientation. A cluster of acids (GluL212, AspL210, and L213) and SerL223 near QB play important roles. A simplified view shows this cluster with a single negative charge (on AspL213 with a hydrogen bond to SerL233) in the ground state. In the QB- state the cluster still has one negative charge, now on the more distant AspL210. AspL213 and SerL223 move so SerL223 can hydrogen bond to QB-. These rearrangements plus other changes throughout the protein make the reaction energetically favorable.     

Simulating proton translocations in proteins: probing proton transfer pathways in the Rhodobacter sphaeroides reaction center.

A general method for simulating proton translocations in proteins and for exploring the role of different proton transfer pathways is developed and examined. The method evaluates the rate constants for proton transfer processes using the energetics of the relevant proton configurations. The energies (DeltaG((m))) of the different protonation states are evaluated in two steps. First, the semimicroscopic version of the protein dipole Langevin dipole (PDLD/S) method is used to evaluate the intrinsic energy of bringing the protons to their protein sites, when the charges of all protein ionized residues are set to zero. Second, the interactions between the charged groups are evaluated by using a Coulomb's Law with an effective dielectric constant. This approach, which was introduced in an earlier study by one of the authors of the current report, allows for a very fast determination of any DeltaG((m)) and for practical evaluation of the time-dependent proton population: That is, the rate constants for proton transfer processes are evaluated by using the corresponding DeltaG((m)) values and a Marcus type relationship. These rate constants are then used to construct a master equation, the integration of which by a fourth-order Runge-Kutta method yields the proton population as a function of time. The integration evaluates, 'on the fly,' the changes of the rate constants as a result of the time-dependent changes in charge-charge interaction, and this feature benefits from the fast determination of DeltaG((m)). The method is demonstrated in a preliminary study of proton translocation processes in the reaction center of Rhodobacter sphaeroides. It is found that proton transfer across water chains involves significant activation barriers and that ionized protein residues probably are involved in the proton transfer pathways. The potential of the present method in analyzing mutation experiments is discussed briefly and illustrated. The present study also examines different views of the nature of proton translocations in proteins. It is shown that such processes are controlled mainly by the electrostatic interaction between the proton site and its surroundings rather than by the local bond rearrangements of water molecules that are involved in the proton pathways. Thus, the overall rate of proton transport frequently is controlled by the highest barrier along the conduction pathway. Proteins 1999;36:484-500.     

Blue light drives B-side electron transfer in bacterial photosynthetic reaction centers.

The core of the photosynthetic reaction center from the purple non-sulfur bacterium Rhodobacter sphaeroides is a quasi-symmetric heterodimer, providing two potential pathways for transmembrane electron transfer. Past measurements have demonstrated that only one of the two pathways (the A-side) is used to any significant extent upon excitation with red or near-infrared light. Here, it is shown that excitation with blue light into the Soret band of the reaction center gives rise to electron transfer along the alternate or B-side pathway, resulting in a charge-separated state involving the anion of the B-side bacteriopheophytin. This electron transfer is much faster than normal A-side transfer, apparently occurring within a few hundred femtoseconds. At low temperatures, the B-side charge-separated state is stable for at least 1 ns, but at room temperature, the B-side bacteriopheophytin anion is short-lived, decaying within approximately 15 ps. One possible physiological role for B-side electron transfer is photoprotection, rapidly quenching higher excited states of the reaction center.     

Protein modifications affecting triplet energy transfer in bacterial photosynthetic reaction centers.

The efficiency of triplet energy transfer from the special pair (P) to the carotenoid (C) in photosynthetic reaction centers (RCs) from a large family of mutant strains has been investigated. The mutants carry substitutions at positions L181 and/or M208 near chlorophyll-based cofactors on the inactive and active sides of the complex, respectively. Light-modulated electron paramagnetic resonance at 10 K, where triplet energy transfer is thermally prohibited, reveals that the mutations do not perturb the electronic distribution of P. At temperatures > or = 70 K, we observe reduced signals from the carotenoid in most of the RCs with L181 substitutions. In particular, triplet transfer efficiency is reduced in all RCs in which a lysine at L181 donates a sixth ligand to the monomeric bacteriochlorophyll B(B). Replacement of the native Tyr at M208 on the active side of the complex with several polar residues increased transfer efficiency. The difference in the efficiencies of transfer in the RCs demonstrates the ability of the protein environment to influence the electronic overlap of the chromophores and thus the thermal barrier for triplet energy transfer.     

Pressure effects on the photochemistry of bacterial photosynthetic reaction centers from Rhodobacter sphaeroides R-26 and Rhodopseudomonas viridis

Electron-transfer reactions and triplet decay rates have been studied at pressures up to 300 MPa. In reaction centers from Rhodobacter sphaeroides R-26, high pressure hastened the electron transfers from both the primary and secondary quinones (Q_A and Q_B) to the primary electron donor bacteriochlorophyll, P. Motion of Q_A between two sites, one nearer to P and the other nearer to Q_B, could account for these pressure effects. In reaction centers from Rhodopseudomonas viridis, charge recombination was slowed by high pressure. Decay rates were also studied for the triplet state, P^R. In Rb. sphaeroides R-26 with Q_A reduced with Na₂S₂O₄, the decay was hastened by pressure. This could be explained if P^R decays through a charge-transfer triplet state, or if the decay kinetics of P^R are sensitive to the distance between P and Q_A⁻. In Rps. viridis reaction centers, and in Rb. sphaeroides reaction centers that were depleted of Q_A, the lifetime of P^R was not altered by pressure.     

Characterization of protein matrix motions in the Rb. sphaeroides photosynthetic reaction center

We use Normal Mode Analysis to investigate motions in the photosynthetic reaction center (RC) protein. We identify the regions involved in concerted fluctuations of the protein matrix and analyze the normalized amplitudes and the directionality of the first few dominant modes. We also seek to quantify the coupling of normal modes to long-range electron transfer (ET). We find that a quasi-continuous spectrum of protein motions rather than one individual mode contributes to light-driven electron transfer. This is consistent with existing theoretical models (e.g. the spin-boson/dispersed polaron model) for the coupling of the protein and solvent "bath" to charge separation events. [Figure: see text].     

A picosecond circular dichroism study of photosynthetic reaction centers from Rhodobacter sphaeroides

Picosecond transient circular dichroism spectra are reported for the primary intermediates in the photocycle of reaction centers isolated from Rhodobacter sphaeroides. The time-resolved circular dichroism spectra of the two electron transfer intermediates (BChl2) +BPh-LQA and (BChl2) +BPhLQ-A reveal a large, nonconservative, and fairly stationary CD band at 800 nm. These results suggests that mechanisms other than exciton interactions need to be included in order to explain the optical activity of this biological system.     

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⁺Q_A ^-Q_BD⁺Q_AQ_B (k _AB) is slowed 3 fold in the IM(L229) and YG(L222) RCs (pH 8). The stabilization of D⁺Q_AQ_B ^- with respect to D⁺Q_AQ_B ^- (pH 8) was found to be eliminated in the IM(L229) mutant RCs (G⁰ 0 meV), was partially reduced in the SP(L223) mutant RCs (G⁰=–30 meV), and was unaltered in the YG(L222) mutant RCs (G⁰=–60 meV), compared to that observed in the native RCs (G⁰=–60 meV). The pH dependences of the charge recombination rate D⁺Q_AQ_B ^-DQ_AQ_B (k _BD) and the electron transfer from Q_A ^- (k _QA ^-Q_A) suggest that the mutations do not affect the protonation state of Glu-L212 nor the electrostatic interactions of Q_B and Q_B ^- with Glu-L212. The binding affinities of UQ₁₀ for the Q_B 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.Abbreviations Bchl bacteriochlorophyll - Bphe bacteriopheophytin - cholate 3,7,12-trihydroxycholanic acid - D donor (bacteriochlorophyll dimer) - EDTA ethylenediamine tetraacetic acid - Fe²⁺ non-heme iron atom - LDAO lauryl dimethylamine oxide - PS II photosystem II - Q_A and Q_B primary and secondary quinone acceptors - RC bacterial reaction center - Tris tris(hydroxymethyl)aminomethane - UQ₀ 2,3-dimethoxy-5-methyl benzoquinone - UQ₁₀ ubiquinone 50     

On the depletion and reconstitution of both QA and metal in reaction centers of the photosynthetic bacterium Rb. sphaeroides R-26

Four possible ways to prepare Q_A-depleted, Fe-depleted and Q_A-reconstituted RCs were studied: (1) first depleting the Fe, then depleting Q_A and finally reconstituting Q_A (D-Fe, D-Q, R-Q), (2) first depleting Q_A, then depleting the Fe and finally reconstituting Q_A (D-Q, D-Fe, R-Q), (3) first depleting Q_A, then reconstituting Q_A and finally depleting Fe (D-Q, R-Q, D-Fe), (4) first depleting Q_A, then depleting the Fe and reconstituting Q_A in the same step (D-Q, D-Fe-R-Q). Our results showed that: method (1) results in the irreversible loss of photochemical activity; method (2) and (3) result in low recovery of the photochemical activity and poor yield of Fe-depleted, Q_A-reconstituted RCs; method (4) gives surprisingly good results. This method allows for the first time to prepare the Q_A-depleted, Fe-depleted, Q_A-reconstituted RCs with high recovery of the photochemical activity and good yield. The sample has 98% of photochemical activity (yield of P⁺ Q_A ^-) compared with that of the native RCs and shows strong polarization of the EPR signal of Q_A ^- under continuous illumination at 5K. The decay halftime of I^- is slow (5 ns) compared with that of the native RCs, but it is the same as that measured for the RCs from which only iron is removed. These results indicate that the depletion of iron and the reconstitution of Q_A have been successful. Reconstitution of the Q_A-depleted, Fe-depleted and Q_A-reconstituted RCs with Zn²⁺ gives also the spin-polarized Q_A ^-, and yields the same decay of I^- (halftime 200 ps) as that of the native RCs.Abbreviations LDAO lauryldimethylamine N-oxide - EDTA ethylenediaminetetraacetic acid - BSA albumin bovine - TL buffer 10 mM Tris.HCl, 0.1% LDAO and 0.1 mM EDTA     

The dynamics of the non-heme iron in bacterial reaction centers from Rhodobacter sphaeroides

We investigate the dynamical properties of the non-heme iron (NHFe) in His-tagged photosynthetic bacterial reaction centers (RCs) isolated from Rhodobacter (Rb.) sphaeroides. M?ssbauer spectroscopy and nuclear inelastic scattering of synchrotron radiation (NIS) were applied to monitor the arrangement and flexibility of the NHFe binding site. In His-tagged RCs, NHFe was stabilized only in a high spin ferrous state. Its hyperfine parameters (IS=1.06±0.01mm/s and QS=2.12±0.01mm/s), and Debye temperature (θ(D0)~167K) are comparable to those detected for the high spin state of NHFe in non-His-tagged RCs. For the first time, pure vibrational modes characteristic of NHFe in a high spin ferrous state are revealed. The vibrational density of states (DOS) shows some maxima between 22 and 33meV, 33 and 42meV, and 53 and 60meV and a very sharp one at 44.5meV. In addition, we observe a large contribution of vibrational modes at low energies. This iron atom is directly connected to the protein matrix via all its ligands, and it is therefore extremely sensitive to the collective motions of the RC protein core. A comparison of the DOS spectra of His-tagged and non-His-tagged RCs from Rb. sphaeroides shows that in the latter case the spectrum was overlapped by the vibrations of the heme iron of residual cytochrome c(2), and a low spin state of NHFe in addition to its high spin one. This enabled us to pin-point vibrations characteristic for the low spin state of NHFe.     

Cu2+ site in photosynthetic bacterial reaction centers from Rhodobacter sphaeroides, Rhodobacter capsulatus, and Rhodopseudomonas viridis

The interaction of metal ions with isolated photosynthetic reaction centers (RCs) from the purple bacteria Rhodobacter sphaeroides, Rhodobacter capsulatus, and Rhodopseudomonas viridis has been investigated with transient optical and magnetic resonance techniques. In RCs from all species, the electrochromic response of the bacteriopheophytin cofactors associated with Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron transfer is slowed in the presence of Cu(2+). This slowing is similar to the metal ion effect observed for RCs from Rb. sphaeroides where Zn(2+) was bound to a specific site on the surface of the RC [Utschig et al. (1998) Biochemistry 37, 8278]. The coordination environments of the Cu(2+) sites were probed with electron paramagnetic resonance (EPR) spectroscopy, providing the first direct spectroscopic evidence for the existence of a second metal site in RCs from Rb. capsulatus and Rps. viridis. In the dark, RCs with Cu(2+) bound to the surface exhibit axially symmetric EPR spectra. Electron spin echo envelope modulation (ESEEM) spectral results indicate multiple weakly hyperfine coupled (14)N nuclei in close proximity to Cu(2+). These ESEEM spectra resemble those observed for Cu(2+) RCs from Rb. sphaeroides [Utschig et al. (2000) Biochemistry 39, 2961] and indicate that two or more histidines ligate the Cu(2+) at the surface site in each RC. Thus, RCs from Rb. sphaeroides, Rb. capsulatus, and Rps. viridis each have a structurally analogous Cu(2+) binding site that is involved in modulating the Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron-transfer process. Inspection of the Rps. viridis crystal structure reveals four potential histidine ligands from three different subunits (M16, H178, H72, and L211) located beneath the Q(B) binding pocket. The location of these histidines is surprisingly similar to the grouping of four histidine residues (H68, H126, H128, and L211) observed in the Rb. sphaeroides RC crystal structure. Further elucidation of these Cu(2+) sites will provide a means to investigate localized proton entry into the RCs of Rb. capsulatus and Rps. viridis as well as locate a site of protein motions coupled with electron transfer.     

Mössbauer spectroscopy studies of photosynthetic reaction centers from Rhodopseudomonas sphaeroides R-26

⁵⁷Fe Mössbauer spectroscopy measurements on reaction centers differing in ubiquinone content, detergent, oxidation state, or the presence of o-phenanthroline all show a single quadrupole doublet of similar splitting (ΔE_Q), center shift (δ) and temperature dependence. The results are indicative of high-spin Fe²⁺ with an approximately invariant first coordination sphere. A crystal field model with strong electron delocalization can account for the temperature dependence of ΔE_Q, but further data are needed to achieve a unique parameterization.     

Protein structure,electron transfer and evolution of prokaryotic photosynthetic reaction centers

Photosynthetic reaction centers from a variety of organisms have been isolated and characterized. The groups of prokaryotic photosynthetic organisms include the purple bacteria, the filamentous green bacteria, the green sulfur bacteria and the heliobacteria as anoxygenic representatives as well as the cyanobacteria and prochlorophytes as oxygenic representatives. This review focuses on structural and functional comparisons of the various groups of photosynthetic reaction centers and considers possible evolutionary scenarios to explain the diversity of existing photosynthetic organisms.Abbreviations BChl bacteriochlorophyll - Chl chlorophyll - Rb Rhodobacter - Rp Rhodopseudomonas