Thermodynamic properties of the reaction center of Rhodopseudomonas viridis in vivo measurement of the reaction center bacteriochlorophyll-primary acceptor intermediary electron carrier

The thermodynamic properties of redox components associated with the reaction center of Rhodopseudomonas viridis have been characterized with respect to their midpoint potentials and relationship with protons. In particular a midpoint potential for the intermediary electron carrier acting between the reaction center bacteriochlorophyll and the primary acceptor has been determined. The rationale for this measurement was that the light-induced triplet/biradical EPR signal would not be observed if this intermediate was chemically reduced before activation. The midpoint potential of the intermediary at pH 10.8 is about −400 mV (n = 1).     

The acceptor quinone complex of Rhodopseudomonas viridis reaction centers

The acceptor complex of isolated reaction centers from Rhodopseudomonas viridis contains both menaquinone and ubiquinone. In a series of flashes the ubiquinone was observed to undergo binary oscillations in the formation and disappearance of a semiquinone, indicative of secondary acceptor (QB) activity. The oscillating signal, Q-B, was typical of a ubisemiquinone anion with a peak at 450 nm (delta epsilon = 6 mM-1 X cm-1) and a shoulder at 430 nm. Weak electrochromic bandshifts in the infrared were also evident. The spectrum of the reduced primary acceptor (Q-A) exhibited a major peak at 412 nm (delta epsilon = 10 mM-1 X cm-1) consistent with the assignment of menaquinone as QA. The Q-A spectrum also had minor peaks at 385 and 455 nm in the blue region. The same spectrum was recorded after quantitative removal of the secondary acceptor, when only menaquinone was present in the reaction centers. Spectral features in the near-infrared due to Q-A were attributed to electrochromic effects on bacteriochlorophyll (BChl) b and bacteriopheophytin (BPh) b pigments resulting in a distinctive split peak at 810 and 830 nm (delta epsilon = 8 mM-1 X cm-1). The menaquinone was identified as 2-methyl-3-nonylisoprenyl-1,4-naphthoquinone (menaquinone-9). The native QA activity was uniquely provided by this menaquinone and ubiquinone was not involved. QB activity, on the other hand, displayed at least a 40-fold preference for ubiquinone (Q-10) as compared to menaquinone. Thus, both quinone-binding sites display remarkable specificity for their respective quinones. In the absence of donors to P+, charge recombination of the P+Q-A and P+Q-B pairs had half-times of 1.1 +/- 0.2 and 110 +/- 20 ms, respectively, at pH 9.0, indicating an electron-transfer equilibrium constant (Kapp2) of at least 100 for Q-AQB in equilibrium QAQ-B. Also observed was a slow recombination of the cytochrome c-558+ Q-A pair, with t 1/2 = 2 +/- 0.5 s at pH 6.     

Spectroscopic properties of the intermediary electron carrier in the reaction center of Rhodopseudomonas viridis evidence for its interaction with the primary acceptor

The spectroscopic properties of the intermediary electron carrier (I), which functions between the bacteriochlorophyll dimer, (BChl)₂, and the primary acceptor quinone · iron, QFe, have been characterized in Rhodopseudomonas viridis. Optically the reduction of I is accompanied by a bleaching of bands at 545 and 790 nm and a broad absorbance increase around 680 nm which we attribute to the reduction of a bacteriopheophytin, together with apparent blue shifts of the bacteriochlorophyll bands at 830 and possibly at 960 nm. Low temperature electron paramagnetic resonance analysis also reveals complicated changes accompanying the reduction of I. In chromatophores I? is revealed as a broad split signal centered close to g 2.003, which is consistent with I? interacting, via exchange coupling and dipolar effects, with the primary acceptor Q?Fe. This is supported by experiments with reaction centers prepared with sodium dodecyl sulfate, which lack the Q?Fe g 1.82 signal, and also lack the broad split I? signal; instead, I? is revealed as an approximately 13 gauss wide free radical centered close to g 2.003. Reaction centers prepared using lauryl dimethylamine N-oxide retain most of their Q?Fe g 1.82 signal, and in this case I? occurs as a mixture of the two EPR signals described above. However, the optical changes accompanying the reduction of I? are very similar in the two reaction center preparations, so we conclude that there is no direct correlation between the two optical and the two EPR signals of I?. Perhaps the simplest explanation of the results is that the two EPR signals reflect the reduced bacteriopheophytin either interacting, or not interacting, with Q?Fe, while the optical changes reflect the reduction of bacteriophenophytin, together with secondary, perhaps electrochromic effects on the bacteriochlorophylls of the reaction center. However, we are unable to eliminate completely the possibility that there is also some electron sharing between the reduced bacteriopheophytin and bacteriochlorophyll.     

Calculated coupling of electron and proton transfer in the photosynthetic reaction center of Rhodopseudomonas viridis.

Based on new Rhodopseudomonas (Rp.) viridis reaction center (RC) coordinates with a reliable structure of the secondary acceptor quinone (QB) site, a continuum dielectric model and finite difference technique have been used to identify clusters of electrostatically interacting ionizable residues. Twenty-three residues within a distance of 25 A from QB (QB cluster) have been shown to be strongly electrostatically coupled to QB, either directly or indirectly. An analogous cluster of 24 residues is found to interact with QA (QA cluster). Both clusters extend to the cytoplasmic surface in at least two directions. However, the QB cluster differs from the QA cluster in that it has a surplus of acidic residues, more strong electrostatic interactions, is less solvated, and experiences a strong positive electrostatic field arising from the polypeptide backbone. Consequently, upon reduction of QA or QB, it is the QB cluster, and not the QA cluster, which is responsible for substoichiometric proton uptake at neutral pH. The bulk of the changes in the QB cluster are calculated to be due to the protonation of a tightly coupled cluster of the three Glu residues (L212, H177, and M234) within the QB cluster. If the lifetime of the doubly reduced state QB2- is long enough, Asp M43 and Ser L223 are predicted to also become protonated. The calculated complex titration behavior of the strongly interacting residues of the QB cluster and the resulting electrostatic response to electron transfer may be a common feature in proton-transferring membrane protein complexes.     

Kinetic properties of the acceptor quinone complex in Rhodopseudomonas viridis

The kinetics of electron transfer from the primary (QA) to the secondary (QB) quinone acceptor in whole cells and chromatophores of Rhodopseudomonas viridis was studied as a function of the redox state of QB and of pH by using a photovoltage technique. Under conditions where QB was oxidized, the reoxidation of QA- was found to be essentially monophasic and independent of pH with a half-time of about 20 microseconds. When QB was reduced to the semiquinone form by a preflash, the reoxidation of QA- was slowed down showing a half-time between 40 and 80 microseconds at pH less than or equal to 9. Above pH 9, the rate of the second electron transfer decreased nearly one order of magnitude per pH unit. After a further preflash, the fast and pH-independent kinetics of QA- reoxidation was essentially restored. The concentration of QA still reduced 100 microseconds after its complete reduction by a flash showed distinct binary oscillations as a function of the number of preflashes, confirming the interpretation that the electron-transfer rate depends on the redox state of QB. After addition of o-phenanthroline, the reoxidation of QA- is slowed down to the time range of seconds as expected for a back-reaction with oxidized cytochrome. Under conditions where inhibitors of the electron transfer between the quinones fail to block this reaction in a fraction of the reaction centers due to the presence of the extremely stable and strongly bound semiquinone, QB-, these reaction centers show a slow electron transfer on the first flash and a fast one on the second, i.e., an out-of-phase oscillation.(ABSTRACT TRUNCATED AT 250 WORDS)     

Microaerophilic growth and induction of the photosynthetic reaction center in Rhodopseudomonas viridis.

Rhodopseudomonas viridis was grown in liquid culture at 30 degrees C anaerobically in light (generation time, 13 h) and under microaerophilic growth conditions in the dark (generation time, 24 h). The bacterium could be cloned at the same temperature anaerobically in light (1 week) and aerobically in the dark (3 to 4 weeks) if oxygen was limited to 0.1%. Oxygen could not be replaced by dimethyl sulfoxide, potassium nitrate, or sodium nitrite as a terminal electron acceptor. No growth was observed anaerobically in darkness or in the light when air was present. A variety of additional carbon sources were used to supplement the standard succinate medium, but enhanced stationary-phase cell density was observed only with glucose. Conditions for induction of the photosynthetic reaction center upon the change from microaerophilic to phototrophic growth conditions were investigated and optimized for a mutant functionally defective in phototrophic growth. R. viridis consumed about 20-fold its cell volume of oxygen per hour during respiration. The MICs of ampicillin, kanamycin, streptomycin, tetracycline, 1-methyl-3-nitro-1-nitrosoguanidine, and terbutryn were determined.     

A system for site-specific mutagenesis of the photosynthetic reaction center in Rhodopseudomonas viridis.

The purple non-sulfur bacterium Rhodopseudomonas viridis contains a photosynthetic reaction center which has been structurally resolved to 2.3 A providing a unique basis for the study of biological electron transfer processes by the method of site-specific mutagenesis. Here we report the construction of a puf operon deleted mutant strain incapable of photosynthetic growth. The deletion was introduced with the help of a newly constructed suicide vector by electroporation which is with conjugation another gene transfer system for R. viridis. The deletion strain was complemented by conjugational gene transfer with wild-type (WT) and mutated LM genes of the puf operon. The complemented WT and mutations YL162F and HL153F grew photosynthetically, expressed and assembled the four subunits L, M, H and Cyt c of the reaction center correctly. These first mutations already demonstrate the value of the R. viridis system for a detailed structure-function analysis of photosynthetic electron transfer.     

EPR and optical spectroscopic properties of the electron carrier intermediate between the reaction center bacteriochlorophylls and the primary acceptor in Chromatium vinosum.

1. A reaction center-cytochrome c complex has been isolated from Chromatium vinosum which is capable of normal photochemistry and light-activated rapid cytochrome c553 and c555 oxidation, but which has no antenna bacteriochlorophyll. As is found in whole cells, ferrocytochrome c553 is oxidized irreversibly in milliseconds by light at 7 K. 2. Room temperature redox potentiometry in combination with EPR analysis at 7 K, of cytochrome c553 and the reaction center bacteriochlorophyll dimer (BChl)2 absorbing at 883 nm yields identical results to those previously reported using optical analytical techniques at 77 K. It shows directly that two cytochrome c553 hemes are equivalent with respect to the light induced (BChl)2+. At 7 K, only one heme can be rapidly oxidized in the light, commensurate with the electron capacity of the primary acceptor (quinone-iron) being unity. 3. Prior chemical reduction of the quinone-iron followed by illumination at 200K, however, leads to the slow (t1/2 approximately equal to 30 s) oxidation of one cytochrome c553 heme, with what appears to be concommitant reduction of one of the two bacteriophytins (BPh) of the reaction center as shown by bleaching of the 760 nm band, a broad absorbance increase at approx. 650 nm and a bleaching at 543 nm. The 800 nm absorbing bacteriochlorophyll is also involved since there is also bleaching at 595 and 800 nm; at the latter wave-length the remaining unbleached band appears to shift significantly to the blue. No redox changes in the 883 absorbing bacteriochlorophyll dimer are seen during or after illumination under these conditions. The reduced part of the state represents what is considered to be the reduced form of the electron carrier (I) which acts as an intermediate between the bacteriochlorophyll dimer and quinone-iron. The state (oxidized c553/reduced I) relaxes in the dark at 200K in t1/2 approx. 20 min but below 77 K it is trapped on a days time scale. 4. EPR analysis of the state trapped as described above reveals that one heme equivalent of cytochrome becomes oxidized for the generation of the state, a result in agreement with the optical data. Two prominent signals are associated with the trapped state in the g = 2 region, which can be easily resolved with temperature and microwave power saturation: one has a line width of 15 g and is centered at g = 2.003; the other, which is the major signal, is also a radical centered at g = 2.003 but is split by 60 G and behaves as though it were an organic free-radical spin-coupled with another paramagnetic center absorbing at higher magnetic field values; this high field partner could be the iron-quinone of the primary acceptor. The identity of two signals associated with I-. is consistent with the idea that the reduced intermediary carrier is not simply BPh-. but also involves a second radical, perhaps the 800 nm bacteriochlorophylls in the reduced state...     

Some experiments on the primary electron acceptor in reaction centres from Rhodopseudomonas sphaeroides.

The bacterial reaction center absorbance change at 450 nm (A-450) assigned to an anionic semiquinone, has been suggested as a candidate for the reduced form of the primary electron acceptor in bacterial photosynthesis. In reaction centers of Rhodopseudomonas sphaeroides we have found kinetic discrepancies between the decay of A-450 and the recovery of photochemical competence. In addition, no proton uptake is measurable on the first turnover, although subsequent ones elicit one proton bound per electron. These results are taken to indicate that the acceptor reaction after a long dark period may be different for the first turnover than for subsequent ones. It is suggested that A-450 is still a likely candidate for the acceptor function but that in reaction centers, additional quinone may act as an adventitious primary acceptor when the "true" primary acceptor is reduced. Alternatively, the primary acceptor may act in a "ping-pong" fashion with respect to subsequent photoelectrons.     

Uphill electron transfer in the tetraheme cytochrome subunit of the Rhodopseudomonas viridis photosynthetic reaction center: evidence from site-directed mutagenesis

The cytochrome (cyt) subunit of the photosynthetic reaction center from Rhodopseudomonas viridis contains four heme groups in a linear arrangement in the spatial order heme1, heme2, heme4, and heme3. Heme3 is the direct electron donor to the photooxidized primary electron donor (special pair, P(+)). This heme has the highest redox potential (E(m)) among the hemes in the cyt subunit. The E(m) of heme3 has been specifically lowered by site-directed mutagenesis in which the Arg residue at the position of 264 of the cyt was replaced by Lys. The mutation decreases the E(m) of heme3 from +380 to +270 mV, i.e., below that of heme2 (+320 mV). In addition, a blue shift of the alpha-band was found to accompany the mutation. The assignment of the lowered E(m) and the shifted alpha-band to heme3 was confirmed by spectroscopic measurements on RC crystals. The structure of the mutant RC has been determined by X-ray crystallography. No remarkable differences were found in the structure apart from the mutated residue itself. The velocity of the electron transfer (ET) from the tetraheme cyt to P(+) was measured under several redox conditions by following the rereduction of P(+) at 1283 nm after a laser flash. Heme3 donates an electron to P(+) with t(1/2) = 105 ns, i.e., faster than in the wild-type reaction center (t(1/2) = 190 ns), as expected from the larger driving force. The main feature is that a phase with t(1/2) approximately 2 micros dominates when heme3 is oxidized but heme2 is reduced. We conclude that the ET from heme2 to heme3 has a t(1/2) of approximately 2 micros, i.e., the same as in the WT, despite the fact that the reaction is endergonic by 50 meV instead of exergonic by 60 meV. We propose that the reaction kinetics is limited by the very uphill ET from heme2 to heme4, the DeltaG degrees of which is about the same (+230 meV) in both cases. The interpretation is further supported by measurements of the activation energy (216 meV in the wild-type, 236 meV in the mutant) and by approximate calculations of ET rates. Altogether these results demonstrate that the ET from heme2 to heme3 is stepwise, starting with a first very endergonic step from heme2 to heme4.     

Conformational heterogeneity of the bacteriopheophytin electron acceptor HA in reaction centers from Rhodopseudomonas viridis revealed by Fourier transform infrared spectroscopy and site-directed mutagenesis.

The light-induced Fourier transform infrared (FTIR) difference spectra corresponding to the photoreduction of either the HA bacteriopheophytin electron acceptor (HA-/HA spectrum) or the QA primary quinone (QA-/QA spectrum) in photosynthetic reaction centers (RCs) of Rhodopseudomonas viridis are reported. These spectra have been compared for wild-type (WT) RCs and for two site-directed mutants in which the proposed interactions between the carbonyls on ring V of HA and the RC protein have been altered. In the mutant EQ(L104), the putative hydrogen bond between the protein and the 9-keto C=O of HA should be affected by changing Glu L104 to a Gln. In the mutant WF(M250), the van der Waals interactions between Trp M250 and the 10a-ester C=O of HA should be modified. The characteristic effects of both mutations on the FTIR spectra support the proposed interactions and allow the IR modes of the 9-keto and 10a-ester C=O of HA and HA- to be assigned. Comparison of the HA-/HA and QA-/QA spectra leads us to conclude that the QA-/QA IR signals in the spectral range above 1700 cm-1 are largely dominated by contributions from the electrostatic response of the 10a-ester C=O mode of HA upon QA photoreduction. A heterogeneity in the conformation of the 10a-ester C=O mode of HA in WT RCs, leading to three distinct populations of HA, appears to be related to differences in the hydrogen-bonding interactions between the carbonyls of ring V of HA and the RC protein. The possibility that this structural heterogeneity is related to the observed multiexponential kinetics of electron transfer and the implications for primary processes are discussed. The effect of 1H/2H exchange on the QA-/QA spectra of the WT and mutant RCs shows that neither Glu L104 nor any other exchangeable carboxylic residue changes appreciably its protonation state upon QA reduction.     

The binding of triazine herbicides to the photosynthetic reaction center of Rhodopseudomonas viridis. Energy minimization studies.

The binding of six herbicides of the triazine family to the photosynthetic reaction center of Rhodopseudomonas viridis was investigated with energy-minimization techniques, in order to correlate experimental with calculated data. The inhibitors were modeled in the active site according to the X-ray structure analysis of the complex formed between the triazine terbutryn (2-ethylamino-4-t-butylamino-6-methylthio-s-triazine) and the reaction center of R. viridis [Michel, H., Epp. O. & Deisenhofer, J. (1986) EMBO J. 5, 2445-2451]. 40 different energy minimizations were carried out with varying cutoff radii, partial charges on inhibitor atoms and dielectric constants, i.e. 10 different combinations of these were tested. The impact of these parameters on the calculated binding and interaction energy was either examined for all protein/triazine complexes or, in the case of the dielectric constant, a smaller sample was used. The calculated energies are dominated by van der Waals interactions, which change by up to 20% when extending the cutoff radius from 0.8 nm to 1.5 nm. The use of uniform or distance-dependent dielectric constant or partial charges on the inhibitor atoms does not severely influence the resulting structures, but shows a great impact on the calculated energies. In the two groups of triazines, each containing three inhibitors with methoxy or methylthio substituents, correlations of biological and calculated data were found quite often, but only once with all six triazines. The energy-minimized structures were compared and analysed. A third hydrogen bond, not seen in the X-ray analysis of the reaction center/tertubryn complex, was found between the t-butylamino moiety of terbutryn (and equivalent moieties in the other triazines) and the carbonyl oxygen of TyrL222.     

Transfer of light-induced electron-spin polarization from the intermediary acceptor to the prereduced primary acceptor in the reaction center of photosynthetic bacteria.

In reaction centers and chromatophores of photosynthetic bacteria strong light-induced emissive ESR signals have been found, not only after a flash but also under continuous illumination. The signal, with g = 2.0048 and delta Hpp = 7.6 G, is only present under reducing conditions in material in which the primary acceptor, ubiquinone, U and its associated high-spin ferrous ion are magnetically uncoupled. its amplitude under continuous illumination is strongly dependent on light intensity and on microwave power. The emissive signal is attributed to the prereduced primary acceptor, U-, which becomes polarized through transfer of spin polarization by a magnetic exchange interaction with the photoreduced, spin polarized intermediary acceptor, I-. A kinetic model is presented which explains the observed dependence of emissivity on light intensity and microwave power. Applying this analysis to the light saturation data, a value of the exchange rate between I- and U- of 4.10(8) s-1 is derived, corresponding to an exchange interaction of 3--5 G.