Cumulant analysis of charge recombination kinetics in bacterial reaction centers reconstituted into lipid vesicles

The kinetics of charge recombination between the primary photoxidized donor (P(+)) and the secondary reduced quinone acceptor (Q(B)(-)) have been studied in reaction centers (RCs) from the purple photosynthetic bacterium Rhodobacter sphaeroides incorporated into lecithin vesicles containing large ubiquinone pools over the temperature range 275 K = (50 +/- 15) nm). Following these premises, we describe the kinetics of P(+)Q(B)(-) recombination with a truncated cumulant expansion and relate it to P(Q) and to the free energy changes for Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron transfer (DeltaG(AB)(o)) and for quinone binding (DeltaG(bind)(o)) at Q(B). The model accounts well for the temperature and quinone dependence of the charge recombination kinetics, yielding DeltaG(AB)(o) = -7.67 +/- 0.05 kJ mol(-1) and DeltaG(bind)(o) = -14.6 +/- 0.6 kJ mol(-1) at 298 K.     

Thermodynamic properties of the semiquinone and its binding site in the ubiquinol-cytochrome c (c2) oxidoreductase of respiratory and photosynthetic systems

The antimycin-sensitive ubisemiquinone radical (QC) of the ubiquinol-cytochrome c oxidoreductase of submitochondrial particles and chromatophores of Rhodopseudomonas sphaeroides Ga has been studied by a combination of redox potentiometry and EPR spectroscopy. This g = 2.005 radical signal appears at physiological pH values and increases in intensity with increasing pH up to pH 7.6 in submitochondrial particles and pH 9.0 in R. sphaeroides after which its intensity remains unchanged. The Em7 (ubiquinone/quinol) of the signal, estimated from redox titration data is 80 mV for submitochondrial particles, and 150 mV in chromatophores. Each of these values is higher than that of the quinone pool by 20 mV in submitochondrial particles and 60 mV in R. sphaeroides. This indicates that the quinone at the binding site is out of equilibrium with the pool, and that binding site preferentially binds quinol over quinone. Analysis of the shapes of the semiquinone titration curves, taken together with the midpoint elevation, indicates a quinone-binding site: cytochrome c1 stoichiometry of 1:1 in both submitochondrial particles and chromatophores. At its maximal intensity, the semiquinone concentration at the binding site is 0.26 in submitochondrial particles (greater than pH 7.6) and 0.4 in chromatophores (greater than pH 9.0). In both systems, the midpoint of the ubiquinone/ubisemiquinone couple is constant as the pH is raised up to the pH of maximal semiquinone formation whereafter it becomes more negative at the rate of -60 mV/pH unit. The midpoint of the ubisemiquinone/quinol couple, on the other hand, varies by -120 mV/pH unit at pH values up to the transition pH, after which it, too, changes by -60 mV/pH unit. This seemingly anomalous behavior may be explained by invoking a protonated group at or near the quinone-binding site whose pK corresponds to the pH transition point in the quinone/semiquinone/quinol redox chemistry when the site is free or when quinone or quinol occupies the site. This pK is elevated to at least pH 9.0 in submitochondrial particles and 10.5 in R. sphaeroides when semiquinone is bound to the site.     

-deltaG(AB) and pH dependence of the electron transfer from P(+)Q(A)(-)Q(B) toP(+)Q(A)Q(B)(-) in Rhodobacter sphaeroides reaction centers

The electron transfer from the reduced primary quinone (Q(A)(-)) to the secondary quinone (Q(B)) can occur in two phases with a well-characterized 100 micros component (tau(2)) and a faster process occurring in less than 10 micros (tau(1)). The fast reaction is clearly seen when the native ubiquinone-10 at Q(A) is replaced with naphthoquinones. The dependence of tau(1) on the free-energy difference between the P(+)Q(A)(-)Q(B) and P(+)Q(A)Q(B)(-) states (-) and on the pH was measured using naphthoquinones with different electrochemical midpoint potentials as Q(A) in Rhodobacter sphaeroides reaction centers (RCs) and in RCs where - is changed by mutation of M265 in the Q(A) site from Ile to Thr (M265IT). Q(B) was ubiquinone (UQ(B)) in all cases. Electron transfer was measured by using the absorption differences of the naphthosemiquinone at Q(A) and the ubisemiquinone at Q(B) between 390 and 500 nm. As - was changed from -90 to -250 meV tau(1) decreased from 29 to 0.2 micros. The free-energy dependence of tau(1) provides a reorganization energy of 850 +/- 100 meV for the electron transfer from Q(A)(-) to Q(B). The slower reaction at tau(2) is free-energy independent, so processes other than electron transfer determine the observed rate. The fraction of the reaction at tau(1) increases with increasing driving force and is 100% of the reaction when - is approximately 100 meV more favorable than in the native RCs with ubiquinone as Q(A). The fast phase, tau(1), is pH independent from pH 6 to 11 while tau(2) slows above pH 9. As the Q(A) isoprene tail length is increased from 2 to 10 isoprene units the fraction at tau(1) decreases. However, tau(1), tau(2), and the fraction of the reaction in each phase are independent of the tail length of UQ(B).     

Low-temperature interquinone electron transfer in photosynthetic reaction centers from Rhodobacter sphaeroides and Blastochloris viridis: characterization of Q(B)- states by high-frequency electron paramagnetic resonance (EPR) and electron-nuclear double resonance (ENDOR)

High-frequency electron paramagnetic resonance (HF EPR) techniques have been employed to look for localized light-induced conformational changes in the protein environments around the reduced secondary quinone acceptor (Q(B)(-)) in Rhodobacter sphaeroides and Blastochloris viridis RCs. The Q(A)(-) and Q(B)(-) radical species in Fe-removed/Zn-replaced protonated RCs substituted with deuterated quinones are distinguishable with pulsed D-band (130 GHz) EPR and provide native probes of both the low-temperature Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron-transfer event and the structure of trapped conformational substates. We report here the first spectroscopic evidence that cryogenically trapped, light-induced changes enable low-temperature Q(A)(-)Q(B) --> Q(A)Q(B)(-) electron transfer in the B. viridis RC and the first observation of an inactive, trapped P(+)Q(B)(-) state in both R. sphaeroides and B. viridis RCs that does not recombine at 20 K. The high resolution and orientational selectivity of HF electron-nuclear double resonance (ENDOR) allows us to directly probe protein environments around Q(B)(-) for distinct P(+)Q(B)(-) kinetic RC states by spectrally selecting specific nuclei in isotopically labeled samples. No structural differences in the protein structure near Q(B)(-) or reorientation (within 5 degrees ) of Q(B)(-) was observed with HF ENDOR spectra of two states of P(+)Q(B)(-): "active" and "inactive" states with regards to low-temperature electron transfer. These results reveal a remarkably enforced local protein environment for Q(B) in its reduced semiquinone state and suggest that the conformational change that controls reactivity resides beyond the Q(B) local environment.     

Photoreduction of the quinone pool in the bacterial photosynthetic membrane: identification of infrared marker bands for quinol formation

The photoreduction of the quinone (Q) pool in the photosynthetic membrane of the purple bacterium Rhodobacter sphaeroides was investigated by steady-state and time-resolved Fourier transform infrared difference spectroscopy. The results are consistent with the existence of a homogeneous Q pool inside the chromatophore membrane, with a size of around 20 Q molecules per reaction center. IR marker bands for the quinone/quinol (Q/QH(2)) redox couple were recognized. QH(2) bands are identified at 1491, 1470, 1433 and 1388-1375 cm(-1). The 1491 cm(-1) band, which is sensitive to (1)H/(2)H exchange, is assigned to a C-C ring mode coupled to a C-OH mode. A feature at approximately 1743/1720 cm(-1) is tentatively related to a perturbation of the carbonyl modes of phospholipid head groups induced by QH(2) formation. Complex conformational changes of the protein in the amide I and II spectral ranges are also apparent during reduction and reoxidation of the Q pool.     

FTIR spectroscopy of the reaction center of Chloroflexus aurantiacus: photoreduction of the bacteriopheophytin electron acceptor

Mid-infrared spectral changes associated with the photoreduction of the bacteriopheophytin electron acceptor H(A) in reaction centers (RCs) of the filamentous anoxygenic phototrophic bacterium Chloroflexus (Cfl.) aurantiacus are examined by light-induced Fourier transform infrared (FTIR) spectroscopy. The light-induced H(A)(-)/H(A) FTIR (1800-1200cm(-1)) difference spectrum of Cfl. aurantiacus RCs is compared to that of the previously well characterized purple bacterium Rhodobacter (Rba.) sphaeroides RCs. The most notable feature is that the large negative IR band at 1674cm(-1) in Rba. sphaeroides R-26, attributable to the loss of the absorption of the 13(1)-keto carbonyl of H(A) upon the radical anion H(A)(-) formation, exhibits only a very minor upshift to 1675cm(-1) in Cfl. aurantiacus. In contrast, the absorption band of the 131-keto C=O of H(A)(-) is strongly upshifted in the spectrum of Cfl. aurantiacus compared to that of Rba. sphaeroides (from 1588 to 1623cm(-1)). The data are discussed in terms of: (i) replacing the glutamic acid at L104 in Rba. sphaeroides R-26 RCs by a weaker hydrogen bond donor, a glutamine, at the equivalent position L143 in Cfl. aurantiacus RCs; (ii) a strengthening of the hydrogen-bonding interaction of the 131-keto C=O of H(A) with Glu L104 and Gln L143 upon H(A)(-) formation and (iii) a possible influence of the protein dielectric environment on the 131-keto C=O stretching frequency of neutral H(A). A conformational heterogeneity of the 133-ester C=O group of H(A) is detected for Cfl. aurantiacus RCs similar to what has been previously described for purple bacterial RCs.     

Stabilization of charge separation and cardiolipin confinement in antenna-reaction center complexes purified from Rhodobacter sphaeroides

The reaction center-light harvesting complex 1 (RC-LH1) purified from the photosynthetic bacterium Rhodobacter sphaeroides has been studied with respect to the kinetics of charge recombination and to the phospholipid and ubiquinone (UQ) complements tightly associated with it. In the antenna-RC complexes, at 6.5 more than three times smaller than that measured in LH1-deprived RCs. At increasing pH values, for which increases, the deceleration observed in RC-LH1 complexes is reduced, vanishing at pH >11.0. In both systems kinetics are described by a continuous rate distribution, which broadens at pH >9.5, revealing a strong kinetic heterogeneity, more pronounced in the RC-LH1 complex. In the presence of the antenna the Q(A)Q(B)(-) state is stabilized by about 40 meV at 6.511. The phospholipid/RC and UQ/RC ratios have been compared in chromatophore membranes, in RC-LH1 complexes and in the isolated peripheral antenna (LH2). The UQ concentration in the lipid phase of the RC-LH1 complexes is about one order of magnitude larger than the average concentration in chromatophores and in LH2 complexes. Following detergent washing RC-LH1 complexes retain 80-90 phospholipid and 10-15 ubiquinone molecules per monomer. The fractional composition of the lipid domain tightly bound to the RC-LH1 (determined by TLC and (31)P-NMR) differs markedly from that of chromatophores and of the peripheral antenna. The content of cardiolipin, close to 10% weight in chromatophores and LH2 complexes, becomes dominant in the RC-LH1 complexes. We propose that the quinone and cardiolipin confinement observed in core complexes reflects the in vivo heterogeneous distributions of these components. Stabilization of the charge separated state in the RC-LH1 complexes is tentatively ascribed to local electrostatic perturbations due to cardiolipin.     

Site specific labeling of Rhodobacter sphaeroides reaction centers with dye probes for surface pH measurements

Covalently bound pH sensitive dyes are an important tool for characterizing the proteolytic reactions of protein complexes that play key roles in biological energy transduction. Here we demonstrate the feasibility of this method for photosynthetic reaction centers (RCs) for the first time, by the highly selective attachment of two thiol reactive derivatives of fluorescein to the two H subunit cysteines of the photosynthetic RC from Rhodobacter sphaeroides R-26 The pK(a) shifts of the dyes upon binding to the protein and in response to high salt were measured, and interpreted based on the structure of the RC. 2-[(5-fluoresceinyl)aminocarbonyl]ethyl-methanethiosulfonate was attached to Cys H156 and fluorescein-5-maleimide to Cys H234. By following the absorption changes of bound fluorescein (500 nm), and those of the hydrophilic pH indicator 8-hydroxypyrene-1,3,6-tris-sulfonic acid (468 nm), the surface and bulk pH were monitored separately with less than 5% crosstalk. Flash-induced proton uptake and external calibrations by mixing with aliquots of acid were measured in different redox states of the RCs. The results indicate that the charge in the quinone acceptor complex after flash activation (primary quinone acceptor (Q(A))- or secondary quinone acceptor (Q(B))-) has no effect on the surface pH and potential in the vicinity of these two attachment sites, between pH 6.5 and 9. Application of the method to other surface locations is discussed.     

Protein/lipid interaction in the bacterial photosynthetic reaction center: phosphatidylcholine and phosphatidylglycerol modify the free energy levels of the quinones

The role of characteristic phospholipids of native membranes, phosphatidylcholine (PC), phosphatidylglycerol (PG), and cardiolipin (CL), was studied in the energetics of the acceptor quinone side in photosynthetic reaction centers of Rhodobacter sphaeroides. The rates of the first, k(AB)(1), and the second, k(AB)(2), electron transfer and that of the charge recombination, k(BP), the free energy levels of Q(A)(-)Q(B) and Q(A)Q(B)(-) states, and the changes of charge compensating protein relaxation were determined in RCs incorporated into artificial lipid bilayer membranes. In RCs embedded in the PC vesicle, k(AB)(1) and k(AB)(2) increased (from 3100 to 4100 s(-1) and from 740 to 3300 s(-1), respectively) and k(BP) decreased (from 0.77 to 0.39 s(-1)) compared to those measured in detergent at pH 7. In PG, k(AB)(1) and k(BP) decreased (to values of 710 and 0.26 s(-1), respectively), while k(AB)(2) increased to 1506 s(-1) at pH 7. The free energy between the Q(A)(-)Q(B) and Q(A)Q(B)(-) states decreased in PC and PG (DeltaG degrees (Q)A-(Q)B(-->)(Q)A(Q)B- = -76.9 and -88.5 meV, respectively) compared to that measured in detergent (-61.8 meV). The changes of the Q(A)/Q(A)(-) redox potential measured by delayed luminescence showed (1) a differential effect of lipids whether RC incorporated in micelles or vesicles, (2) an altered binding interaction between anionic lipids and RC, (3) a direct influence of PC and PG on the free energy levels of the primary and secondary quinones probably through the intraprotein hydrogen-bonding network, and (4) a larger increase of the Q(A)/Q(A)(-) free energy in PG than in PC both in detergent micelles and in single-component vesicles. On the basis of recent structural data, implications of the binding properties of phospholipids to RC and possible interactions between lipids and electron transfer components will be discussed.     

Primary quinone (QA) binding site of bacterial photosynthetic reaction centers: mutations at residue M265 probed by FTIR spectroscopy

In the primary quinone (Q(A)) binding site of Rb. sphaeroides reaction centers (RCs), isoleucine M265 is in extensive van der Waals contact with the ubiquinone headgroup. Substitution of threonine or serine for this residue (mutants M265IT and M265IS), but not valine (mutant M265IV), lowers the redox midpoint potential of Q(A) by about 100 mV (Takahashi et al. (2001) Biochemistry 40, 1020-1028). The unexpectedly large effect of the polar substitutions is not due to reorientation of the methoxy groups as similar redox potential changes are seen for these mutants with either ubiquinone or anthraquinone as Q(A). Using FTIR spectroscopy to compare Q(A)(-)/Q(A) IR difference spectra for wild type and the M265 mutant RCs, we found changes in the polar mutants (M265IT and M265IS) in the quinone C[double bond]O and C[double bond]C stretching region (1600-1660 cm(-1)) and in the semiquinone anion band (1440-1490 cm(-1)), as well as in protein modes. Modeling the mutations into the X-ray structure of the wild-type RC indicates that the hydroxyl group of the mutant polar residues, Thr and Ser, is hydrogen bonded to the peptide C[double bond]O of Thr(M261). It is suggested that the mutational effect is exerted through the extended backbone region that includes Ala(M260), the hydrogen bonding partner to the C1 carbonyl of the quinone headgroup. The resulting structural perturbations are likely to include lengthening of the hydrogen bond between the quinone C1[double bond]O and the peptide NH of Ala(M260). Possible origins of the IR spectroscopic and redox potential effects are discussed.     

Simultaneous replacement of Asp-L210 and Asp-M17 with Asn increases proton uptake by Glu-L212 upon first electron transfer to QB in reaction centers from Rhodobacter sphaeroides.

In the photosynthetic reaction center (RC) from Rhodobacter sphaeroides, the first electron transfer to the secondary quinone acceptor Q(B) is coupled to the protonation of Glu-L212, located approximately 5 A from the center of Q(B). Upon the second electron transfer to Q(B), Glu-L212 is involved in fast proton delivery to the reduced Q(B). Since Asp-L210 and Asp-M17 play an important role in the proton transfer to the Q(B) site [Paddock, M. L., Adelroth, P., Chang, C., Abresch, E. C., Feher, G., and Okamura, M. Y. (2001) Biochemistry 40, 6893-6902], we investigated the effects of replacing one or both Asp residues with Asn on proton uptake by Glu-L212 using FTIR difference spectroscopy. Upon the first electron transfer to Q(B), the amplitude of the proton uptake by Glu-L212 at pH 8 is increased in the single and double mutant RCs, as is evident from the larger intensity (by 35-55%) of the carboxylic acid band at 1727 cm(-1) in the Q(B)(-)/Q(B) difference spectra of mutant RCs, compared to that at 1728 cm(-1) in native RCs. This implies that the extent of ionization of Glu-L212 in the Q(B) ground state is greater in the mutants than in native RCs and that Asp-M17 and Asp-L210 are at least partially ionized near neutral pH in native RCs. In addition, no changes in the protonation state or the environment of these two residues are detected upon Q(B) reduction. The absence of the 1727 cm(-1) signal in all of the RCs lacking Glu-L212, confirms that the positive band at 1728-1727 cm(-1) probes the protonation of Glu-L212 in native and mutant RCs.     

Effect of metal binding on electrogenic proton transfer associated with reduction of the secondary electron acceptor (QB) in Rhodobacter sphaeroides chromatophores

The influence of metal ion (Cd(2+), Zn(2+), Ni(2+)) binding on the electrogenic phases of proton transfer connected with reduction of quinone Q(B) in chromatophores from Rhodobacter sphaeroides was studied by time-resolved electric potential changes. In the presence of metals, the electrogenic transients associated with proton transfer on first and second flash at pH 8 were found to be slower by factors of 3-6. This is essentially the same effect of metal binding that was observed on optical transients in isolated reaction centers (RC), where the metal ion was shown to inhibit proton transfer [Paddock, M. L., Graige, M. S., Feher, G., and Okamura, M. Y. (1999) Proc. Natl. Acad. Sci. U.S.A. 96, 6183-6188]. The effect of metal binding on the kinetics in chromatophores is, therefore, similarly attributed to inhibition of proton uptake, which becomes rate-limiting. A striking observation was an increase in the amplitude of the electrogenic proton-uptake phase after the first flash with bound metal ion. We attribute this to a loss of internal proton rearrangement, requiring that the protons that stabilize Q(B)(-) come from solution. In mutant RCs, in which His-H126 and His-H128 are replaced with Ala, the apparent binding of Cd(2+) and Ni(2+) was decreased, showing that the binding site of these metal ions is the same as found in RC crystals [Axelrod, H. L., Abresch, E. C., Paddock, M. L., Okamura, M. Y., and Feher, G. (2000) Proc. Natl. Acad. Sci. U.S.A. 97, 1542-1547]. Therefore, the unique proton entry point near His-H126, His-H128, and Asp-M17 that was identified in isolated RCs is also the entry point in chromatophores.     

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.     

Delayed fluorescence from the photosynthetic reaction center measured by electronic gating of the photomultiplier

The decay of the delayed fluorescence (920 nm) of reaction centers from the photosynthetic bacterium Rhodobacter sphaeroides R26 in the P(+)Q(A)(-) charge-separated state (P and Q(A) are the primary donor and quinone, respectively) has been monitored in a wide (100 ns to 100 ms) time range. The photomultiplier (Hamamatsu R3310-03) was protected from the intense prompt fluorescence by application of gating potential pulses (-280 V) to the first, third, and fifth dynodes during the laser pulse. The gain of the photomultiplier dropped transiently by a factor of 1 x 10(6). The delayed fluorescence showed a smooth but nonexponential decay from 100 ns to 1 ms that was explained by the relaxation of the average free energy between P* and P(+)Q(A)(-) changing from -580 to -910 meV. This relaxation is due to the slow protein response to charge separation and can be described by a Kohlrausch relaxation function with time constant of 65 micros and a stretching exponent of alpha = 0.45.     

Fourier transform infrared evidence of proton uptake by glutamate L212 upon reduction of the secondary quinone QB in the photosynthetic reaction center from Rhodobacter capsulatus

The photoreduction of the secondary quinone Q(B) in native reaction centers (RCs) of Rhodobacter capsulatus and in RCs from the GluL212 --> Gln and GluL212 --> Ala mutants has been investigated at pH 7 in (1)H(2)O and (2)H(2)O by light-induced Fourier transform infrared (FTIR) difference spectroscopy. The Q(B)(-)/Q(B) FTIR difference spectra reflect changes of quinone-protein interactions and of protonation state of carboxylic acid groups as well as reorganization of the protein upon electron transfer. Comparison of Q(B)(-)/Q(B) spectra of native and mutant RCs indicates that the interactions between Q(B) or Q(B)(-) and the protein are similar in all RCs. A differential signal at approximately 1650/1640 cm(-1), which is common to all the spectra, is associated with a movement of a peptide carbonyl or a side chain following Q(B) reduction. On the other hand, Q(B)(-)/Q(B) spectra of native and mutant RCs display several differences, notably between 1700 and 1650 cm(-1) (amide I and side chains), between 1570 and 1530 cm(-1) (amide II), and at 1728-1730 cm(-1) (protonated carboxylic acid groups). In particular, the latter region in native RCs is characterized by a main positive band at 1728 cm(-1) and a negative signal at 1739 cm(-1). In the L212 mutants, the amplitude of the positive band is strongly decreased leading to a differential signal at 1739/1730 cm(-1) that is insensitive to (1)H/(2)H isotopic exchange. In native RCs, only the 1728 cm(-1) band is affected in (2)H(2)O while the 1739 cm(-1) signal is not. The effects of the mutations and of (1)H/(2)H exchange on the Q(B)(-)/Q(B) spectra concur in the attribution of the 1728 cm(-1) band in native RCs to (partial) proton uptake by GluL212 upon the first electron transfer to Q(B), as previously observed in Rhodobacter sphaeroides RCs [Nabedryk, E., Breton, J., Hienerwadel, R., Fogel, C., M?ntele, W., Paddock, M. L., and Okamura, M. Y. (1995) Biochemistry 34, 14722-14732]. More generally, strong homologies of the Q(B) to Q(B)(-) transition in the RCs from Rb. sphaeroides and Rb. capsulatus are detected by differential FTIR spectroscopy. The FTIR data are discussed in relation with the results from global proton uptake measurements and electrogenic events concomitant with the reduction of Q(B) and with a model of the Q(B) turnover in Rb. sphaeroides RCs [Mulkidjanian, A. Y. (1999) FEBS Lett. 463, 199-204].     

Modulation of the redox state of quinones by light in Rhodobacter sphaeroides under anaerobic conditions

Illumination of intact cells of Rhodobacter sphaeroides under anaerobic conditions has a dual effect on the redox state of the quinone pool. A large oxidation of the quinone pool is observed during the first seconds following the illumination. This oxidation is suppressed by the addition of an uncoupler in agreement with a light-induced reverse electron transfer at the level of the complex I, present both in the non-invaginated part of the membrane and in the chromatophores. At longer dark times, this illumination increases the reducing power of the cells leading to a significant reduction of the others reaction centers (RCs). From the observation that a significant proportion of RCs could be reduced by the preillumination without affecting the numbers of charge separation for the RCs, we conclude that there is no rapid thermodynamic equilibrium between the quinones present in the non-invaginated part of the membrane and those localized in the chromatophores. Under anaerobic conditions where the chromatophores quinone pool is fully reduced, we deduce, on the basis of flash-induced fluorescence kinetics, that the reduced RCs are exclusively reoxidized by the quinone generated at the Q _o site of the cyt bc ₁ complex. The supramolecular association between a dimeric RC-LHI complex and one cyt bc ₁ complex allows the confinement of a quinone between the RC-LHI directly associated to the cyt bc ₁ complex.     

Quinone reduction via secondary B-branch electron transfer in mutant bacterial reaction centers

Symmetry-related branches of electron-transfer cofactors-initiating with a primary electron donor (P) and terminating in quinone acceptors (Q)-are common features of photosynthetic reaction centers (RC). Experimental observations show activity of only one of them-the A branch-in wild-type bacterial RCs. In a mutant RC, we now demonstrate that electron transfer can occur along the entire, normally inactive B-branch pathway to reduce the terminal acceptor Q(B) on the time scale of nanoseconds. The transmembrane charge-separated state P(+)Q(B)(-) is created in this manner in a Rhodobacter capsulatus RC containing the F(L181)Y-Y(M208)F-L(M212)H-W(M250)V mutations (YFHV). The W(M250)V mutation quantitatively blocks binding of Q(A), thereby eliminating Q(B) reduction via the normal A-branch pathway. Full occupancy of the Q(B) site by the native UQ(10) is ensured (without the necessity of reconstitution by exogenous quinone) by purification of RCs with the mild detergent, Deriphat 160-C. The lifetime of P(+)Q(B)(-) in the YFHV mutant RC is >6 s (at pH 8.0, 298 K). This charge-separated state is not formed upon addition of competitive inhibitors of Q(B) binding (terbutryn or stigmatellin). Furthermore, this lifetime is much longer than the value of approximately 1-1.5 s found when P(+)Q(B)(-) is produced in the wild-type RC by A-side activity alone. Collectively, these results demonstrate that P(+)Q(B)(-) is formed solely by activity of the B-branch carriers in the YFHV RC. In comparison, P(+)Q(B)(-) can form by either the A or B branches in the YFH RC, as indicated by the biexponential lifetimes of approximately 1 and approximately 6-10 s. These findings suggest that P(+)Q(B)(-) states formed via the two branches are distinct and that P(+)Q(B)(-) formed by the B side does not decay via the normal (indirect) pathway that utilizes the A-side cofactors when present. These differences may report on structural and energetic factors that further distinguish the functional asymmetry of the two cofactor branches.     

Trapping conformational intermediate states in the reaction center protein from photosynthetic bacteria

In protein, conformational changes are often crucial for function but not easy to observe. Two functionally relevant conformational intermediate states of photosynthetic reaction center protein (RCs) are trapped and characterized at low temperature. RCs frozen in the dark do not allow electron transfer from the reduced primary quinone, Q(A)(-), to the secondary quinone, Q(B). In contrast, RCs frozen under illumination in the product (P(+)Q(A)Q(B)(-)) state, with the oxidized electron donor, P(+), and reduced Q(B)(-), return to the ground state at cryogenic temperature in a conformation that allows a high yield of Q(B) reduction. Thus, RCs frozen under illumination are found to be trapped above the ground state in a conformation that allows product formation. When the temperature is raised above 120 K, the protein relaxes to an inactive conformation which is different from the RCs frozen in the dark. The activation energy for this change is 87 +/- 8 meV, and the active and inactive states differ in energy by only 16 +/- 3 meV. Thus, there are several conformational substates along the reaction coordinate with different transition temperatures. The ground state spectra of the RCs in active and inactive conformations report differences in the intraprotein electrostatic field, demonstrating that the dipole or charge distribution has changed. In addition, the electrochromic shift associated with the Q(A)(-) to Q(B) electron transfer at low temperature was characterized. The electron-transfer rate from Q(B)(-) to P(+) was measured at cryogenic temperature and is similar to the rate at room temperature, as expected for an exothermic, electron tunneling reaction in RCs.     

Redox potential of quinones in photosynthetic reaction centers from Rhodobacter sphaeroides: dependence on protonation of Glu-L212 and Asp-L213

The absolute values of the one-electron redox potentials of the two quinones (Q(A) and Q(B)) in bacterial photosynthetic reaction centers from Rhodobacter sphaeroides were calculated by evaluating the electrostatic energies from the solution of the linearized Poisson-Boltzmann equation at pH 7.0. The redox potential for Q(A) was calculated to be between -173 and -160 mV, which is close to the lowest measured values that are assumed to refer to nonequilibrated protonation patterns in the redox state Q(A)(-). The redox potential of quinone Q(B) is found to be about 160-220 mV larger for the light-exposed than for the dark-adapted structure. These values of the redox potentials are obtained if Asp-L213 is nearly protonated (probability 0.75-1.0) before and after electron transfer from Q(A) to Q(B), while Glu-L212 is partially protonated (probability 0.6) in the initial state Q(A)(-)Q(B)(0) and fully protonated in the final state Q(A)(0)Q(B)(-). Conversely, if the charge state of the quinones is varied from Q(A)(-)Q(B)(0) to Q(A)(0)Q(B)(-) corresponding to the electron transfer from Q(A) to Q(B), Asp-L213 remains protonated, while Glu-L212 changes its protonation state from 0.15 H(+) to fully protonated. In agreement with results from FTIR spectra, there is proton uptake at Glu-L212 going along with the electron transfer, whereas Asp-L213 does not change its protonation state. However, in our simulations Asp-L213 is considered to be protonated rather than ionized as deduced from FTIR spectra. The calculated redox potential of Q(A) shows little dependence on the charge state of Asp-L213, which is due to a strong coupling with the protonation state of Asp-M17 but increases by 50 mV if Glu-L212 changes from the ionized to the protonated charge state. Both are in agreement with fluorescence measurements observing the decay of SP(+)Q(A)(-) in a wide pH regime. The computed difference in redox potential of Q(B) in the light-exposed and dark-adapted structure was traced back to the hydrogen bond of Q(B) with His-L190 that is lost in the dark-adapted structure and the charge of the non-heme iron atom, which is closer to Q(B) in the light-exposed than in the dark-adapted structure.