Direct Evidence for Nitrogen Ligation to the High Stability Semiquinone Intermediate in Escherichia coli Nitrate Reductase A

The membrane-bound heterotrimeric nitrate reductase A (NarGHI) catalyzes the oxidation of quinols in the cytoplasmic membrane of Escherichia coli and reduces nitrate to nitrite in the cytoplasm. The enzyme strongly stabilizes a menasemiquinone intermediate at a quinol oxidation site (Q_D) located in the vicinity of the distal heme b_D. Here molecular details of the interaction between the semiquinone radical and the protein environment have been provided using advanced multifrequency pulsed EPR methods. ¹⁴N and ¹⁵N ESEEM and HYSCORE measurements carried out at X-band (∼9.7 GHz) on the wild-type enzyme or the enzyme uniformly labeled with ¹⁵N nuclei reveal an interaction between the semiquinone and a single nitrogen nucleus. The isotropic hyperfine coupling constant A_iso(¹⁴N) ∼0.8 MHz shows that it occurs via an H-bond to one of the quinone carbonyl group. Using ¹⁴N ESEEM and HYSCORE spectroscopies at a lower frequency (S-band, ∼3.4 GHz), the ¹⁴N nuclear quadrupolar parameters of the interacting nitrogen nucleus (κ = 0.49, η = 0.50) were determined and correspond to those of a histidine N_δ, assigned to the heme b_D ligand His-66 residue. Moreover S-band ¹⁵N ESEEM spectra enabled us to directly measure the anisotropic part of the nitrogen hyperfine interaction (T(¹⁵N) = 0.16 MHz). A distance of ∼2.2 Åbetween the carbonyl oxygen and the nitrogen could then be calculated. Mechanistic implications of these results are discussed in the context of the peculiar properties of the menasemiquinone intermediate stabilized at the Q_D site of NarGHI.     

1,2H hyperfine spectroscopy and DFT modeling unveil the demethylmenasemiquinone binding mode to E. coli nitrate reductase A (NarGHI)

The quinol oxidation site Q_D in E. coli respiratory nitrate reductase A (EcNarGHI) reacts with the three isoprenoid quinones naturally synthesized by the bacterium, i.e. ubiquinones (UQ), menaquinones (MK) and demethylmenaquinones (DMK). The binding mode of the demethylmenasemiquinone (DMSK) intermediate to the EcNarGHI Q_D quinol oxidation site is analyzed in detail using ^1,2H hyperfine (hf) spectroscopy in combination with H₂O/D₂O exchange experiments and DFT modeling, and compared to the menasemiquinone one bound to the Q_D site (MSK_D) previously studied by us. DMSK_D and MSK_D are shown to bind in a similar and strongly asymmetric manner through a short (~1.7 Å) H-bond. The origin of the specific hf pattern resolved on the DMSK_D field-swept EPR spectrum is unambiguously ascribed to slightly inequivalent contributions from two β-methylene protons of the isoprenoid side chain. DFT calculations show that their large isotropic hf coupling constants (A_iso ~12 and 15 MHz) are consistent with both (i) a specific highly asymmetric binding mode of DMSK_D and (ii) a near in-plane orientation of its isoprenyl chain at Cβ relative to the aromatic ring, which differs by ~90° to that predicted for free or NarGHI-bound MSK. Our results provide new insights into how the conformation and the redox properties of different natural quinones are selectively fine-tuned by the protein environment at a single Q site. Such a fine-tuning most likely contributes to render NarGHI as an efficient and flexible respiratory enzyme to be used upon rapid variations of the Q-pool content.     

Local Control Model of Excitation–Contraction Coupling in Skeletal Muscle

The voltage-activated H⁺ selective conductance of rat alveolar epithelial cells was studied using whole-cell and excised-patch voltage-clamp techniques. The effects of substituting deuterium oxide, D₂O, for water, H₂O, on both the conductance and the pH dependence of gating were explored. D⁺ was able to permeate proton channels, but with a conductance only about 50% that of H⁺. The conductance in D₂O was reduced more than could be accounted for by bulk solvent isotope effects (i.e., the lower mobility of D⁺ than H⁺), suggesting that D⁺ interacts specifically with the channel during permeation. Evidently the H⁺ or D⁺ current is not diffusion limited, and the H⁺ channel does not behave like a water-filled pore. This result indirectly strengthens the hypothesis that H⁺ (or D⁺) and not OH⁻ is the ionic species carrying current. The voltage dependence of H⁺ channel gating characteristically is sensitive to pH_o and pH_i and was regulated by pD_o and pD_i in an analogous manner, shifting 40 mV/U change in the pD gradient. The time constant of H⁺ current activation was about three times slower (τ_act was larger) in D₂O than in H₂O. The size of the isotope effect is consistent with deuterium isotope effects for proton abstraction reactions, suggesting that H⁺ channel activation requires deprotonation of the channel. In contrast, deactivation (τ_tail) was slowed only by a factor ≤1.5 in D₂O. The results are interpreted within the context of a model for the regulation of H⁺ channel gating by mutually exclusive protonation at internal and external sites (Cherny, V.V., V.S. Markin, and T.E. DeCoursey. 1995. J. Gen. Physiol. 105:861–896). Most of the kinetic effects of D₂O can be explained if the pK _a of the external regulatory site is ∼0.5 pH U higher in D₂O.     

A reevaluation of the events leading to the electrogenic reaction and proton translocation in the ubiquinol-cytochrome c oxidoreductase of Rhodopseudomonas sphaeroides

Chromatophore membranes from Rhodopseudomonas sphaeroides activated by light display a carotenoid band shift (phase III) that occurs in response to the electrogenic event (charge separation) in the ubiquinol-cytochrome c oxidoreductase. The rate of formation of this electrogenic event has previously been shown to be strongly dependent on the initial redox state of a bound ubiquinone species (designated Q_z) associated with the oxidoreductase. When Q_z is reduced (quinol form; Q_zH₂) the electrogenic event takes place in less than 5 ms. When Q_z is oxidized (quinone form; Q_z) it is much slower; under these conditions the fact that it occurs has been ignored. In this report, we address this issue and describe events that lead to the generation of carotenoid band shift phase III when the total population of Q_z of the chromatophore is oxidized before flash activation. The following characteristics are apparent: (1) When oxidized Q_z is present before activation, the half-time of formation of carotenoid band-shift phase III is 10–20-times slower than when Q_zH₂ is present before activation. (2) When oxidized Q_z is present, the measured full extent of phase III generated by a single-turnover flash is diminished by about one-half of that observed when Q_zH₂ is present before activation. (3) The rate of formation of the carotenoid band shift phase III when Q_z is initially oxidized corresponds closely to the rate of completion of the flash-activated electron-transfer cycle. This can be seen under two different conditions: (a) as the partial reduction of cytochrome c₁ + c₂ (at redox potentials of 200–300 mV) or (b) as the partial reduction of flash-oxidized bacteriochlorophyll dimer, (BChl)₂⁺ (at redox potentials above 300 mV). (4) At the higher redox potentials (above 300 mV), antimycin-sensitive proton binding shares a common, rate-limiting step with the carotenoid band shift phase III and (BChl)₂⁺ reduction. (5) However, proton binding at redox potentials above 300 mV is not observed at all unless valinomycin (K⁺) is present. Thus, proton binding occurs only when the carotenoid band shift is collapsed in milliseconds, whereas, conversely, the carotenoid band shift is stably generated when proton binding is not observed. These and other observations are the basis of a reevaluation of our current views on the coupling of electron transfer and proton translocation in photosynthetic bacteria.     

Evidence for an anisotropic magnetic interaction between the (bacteriopheophytin) intermediary acceptor and the first quinone acceptor in bacterial photosynthesis

We have investigated electron spin polarization effects occurring in protonated and perdeuterated reaction centers of Rhodospirillum rubrum with electron spin resonance at 9 and 35 GHz (X- and Q-band). As for Rhodopseudomonas sphaeroides strains 2.4.1 and R-26 (Gast, P. and Hoff, A.J. (1979) Biochim. Biophys. Acta 548, 520–535; Gast, P., Mushlin, R.A. and Hoff, A.J. (1982) J. Phys. Chem. 86, 2886–2891), electron spin polarization effects of the prereduced first quinone acceptor Q^?_A in R. rubrum are strongly nonuniform. This nonuniformity is due to an anisotropic magnetic coupling between the intermediary bacteriopheophytin acceptor (I^?) and Q^?_A. It is argued that the anisotropy is too strong to arise solely from an anisotropy in the exchange interaction between I^? and Q^?_A and that dipolar contributions to the magnetic coupling between I^? and Q^?_A are important. The anisotropy in the magnetic coupling for reaction centers of Rps. sphaeroides strains 2.4.1 and R-26 is different from that of R. rubrum wild type. The combination of the 4-fold higher resolution at Q-band and the line narrowing upon deuteration has enabled us to obtain the principal g values and two hyperfine interaction constants of the reduced first quinone acceptor Q^?_A. The principal g values are g_x = 2.0067, g_y = 2.0056 and g_z = 2.0024; the hyperfine constant of the CH₂ group at position 1 is 1.6 G and that of the CH₃ group at position 2 is 2.1 G. These values are close to those found for ubisemiquinone in vitro (Okamura, M.Y., Debus, R.J., Isaacson, R.A. and Feher, G. (1980) Fed. Proc. 39, 1802; Hales, B.J. (1975) J. Am. Chem. Soc. 97, 5993–5997).     

Redox potential of the non-heme iron complex in bacterial photosynthetic reaction center

In bacterial photosynthetic reaction centers (bRC), the electron is transferred from the special pair (P) via accessory bacteriochlorophyll (B_A), bacteriopheopytin (H_A), the primary quinone (Q_A) to the secondary quinone (Q_B). Although the non-heme iron complex (Fe complex) is located between Q_A and Q_B, it was generally supposed not to be redox-active. Involvement of the Fe complex in electron transfer (ET) was proposed in recent FTIR studies [A. Remy and K. Gerwert, Coupling of light-induced electron transfer to proton uptake in photosynthesis, Nat. Struct. Biol. 10 (2003) 637-644]. However, other FTIR studies resulted in opposite results [J. Breton, Steady-state FTIR spectra of the photoreduction of Q_A and Q_B in Rhodobacter sphaeroides reaction centers provide evidence against the presence of a proposed transient electron acceptor X between the two quinones, Biochemistry 46 (2007) 4459-4465]. In this study, we calculated redox potentials of Q_A/B (E_m(Q_A/B)) and the Fe complex (E_m(Fe)) based on crystal structure of the wild-type bRC (WT-bRC), and we investigated the energetics of the system where the Fe complex is assumed to be involved in the ET. E_m(Fe) in WT-bRC is much less pH-dependent than that in PSII. In WT-bRC, we observed significant coupling of ET with Glu-L212 protonation upon oxidation of the Fe complex and a dramatic E_m(Fe) downshift by 230 mV upon formation of Q_A⁻ (but not Q_B⁻) due to the absence of proton uptake of Glu-L212. Changes in net charges of the His ligands of the Fe complex appear to be the nature of the redox event if we assume the involvement of the Fe complex in the ET.     

Electron transfer in reaction centers of Rhodopseudomonas sphaeroides. I. Determination of the charge recombination pathway of D+QAQ−B and free energy and kinetic relations between Q−AQB and QAQ−B

The electron-transfer reactions and thermodynamic equilibria involving the quinone acceptor complex in bacterial reaction centers from R. sphaeroides were investigated. The reactions are described by the scheme: We found that the charge recombination pathway of D⁺Q_AQ^?_B proceeds via the intermediate state D⁺Q^?_AQ_B, the direct pathway contributing less than approx. 5% to the observed recombination rate. The method used to obtain this result was based on a comparison of the kinetics predicted for the indirect pathway (given by the product k_AD-times the fraction of reaction centers in the Q^?_AQ_B state) with the observed recombination rate, k^obs_{D⁺ →D}. The kinetic measurements were used to obtain the pH dependence (6.1 ? pH ? 11.7) of the free energy difference between the states Q^?_AQ_B and Q_AQ^?_B. At low pH (less than 9) Q_AQ^?_B is stabilized relative to Q^?_AQ_B by 67 meV, whereas at high pH Q^?_AQ_B is energetically favored. Both Q^?_A and Q^?_B associate with a proton, with pK values of 9.8 and 11.3, respectively. The stronger interaction of the proton with Q^?_B provides the driving force for the forward electron transfer.     

The influence of hydrogen bonds on electron transfer rate in photosynthetic RCs

Hydrogen bonds formed between photosynthetic reaction centers (RCs) and their cofactors were shown to affect the efficacy of electron transfer. The mechanism of such influence is determined by sensitivity of hydrogen bonds to electron density rearrangements, which alter hydrogen bonds potential energy surface. Quantum chemistry calculations were carried out on a system consisting of a primary quinone Q_A, non-heme Fe²⁺ ion and neighboring residues_. The primary quinone forms two hydrogen bonds with its environment, one of which was shown to be highly sensitive to the Q_A state. In the case of the reduced primary quinone two stable hydrogen bond proton positions were shown to exist on [Q_A-His^M219] hydrogen bond line, while there is only one stable proton position in the case of the oxidized primary quinone. Taking into account this fact and also the ability of proton to transfer between potential energy wells along a hydrogen bond, theoretical study of temperature dependence of hydrogen bond polarization was carried out. Current theory was successfully applied to interpret dark P⁺/Q_A⁻ recombination rate temperature dependence.     

Quinone transport in the closed light-harvesting 1 reaction center complex from the thermophilic purple bacterium Thermochromatium tepidum

Redox-active quinones play essential roles in efficient light energy conversion in type-II reaction centers of purple phototrophic bacteria. In the light-harvesting 1 reaction center (LH1-RC) complex of purple bacteria, Q_B is converted to Q_BH₂ upon light-induced reduction and Q_BH₂ is transported to the quinone pool in the membrane through the LH1 ring. In the purple bacterium Rhodobacter sphaeroides, the C-shaped LH1 ring contains a gap for quinone transport. In contrast, the thermophilic purple bacterium Thermochromatium (Tch.) tepidum has a closed O-shaped LH1 ring that lacks a gap, and hence the mechanism of photosynthetic quinone transport is unclear. Here we detected light-induced Fourier transform infrared (FTIR) signals responsible for changes of Q_B and its binding site that accompany photosynthetic quinone reduction in Tch. tepidum and characterized Q_B and Q_BH₂ marker bands based on their ¹⁵N- and ¹³C-isotopic shifts. Quinone exchanges were monitored using reconstituted photosynthetic membranes comprised of solubilized photosynthetic proteins, membrane lipids, and exogenous ubiquinone (UQ) molecules. In combination with ¹³C-labeling of the LH1-RC and replacement of native UQ₈ by ubiquinones of different tail lengths, we demonstrated that quinone exchanges occur efficiently within the hydrophobic environment of the lipid membrane and depend on the side chain length of UQ. These results strongly indicate that unlike the process in Rba. sphaeroides, quinone transport in Tch. tepidum occurs through the size-restricted hydrophobic channels in the closed LH1 ring and are consistent with structural studies that have revealed narrow hydrophobic channels in the Tch. tepidum LH1 transmembrane region.     

Characterization of the exchangeable protons in the immediate vicinity of the semiquinone radical at the QH site of the cytochrome bo3 from Escherichia coli

The cytochrome bo3 ubiquinol oxidase from Escherichia coli resides in the bacterial cytoplasmic membrane and catalyzes the two-electron oxidation of ubiquinol-8 and four-electron reduction of O2 to water. The one-electron reduced semiquinone forms transiently during the reaction, and the enzyme has been demonstrated to stabilize the semiquinone. Two-dimensional electron spin echo envelope modulation has been applied to explore the exchangeable protons involved in hydrogen bonding to the semiquinone by substitution of 1H2O by 2H2O. Three exchangeable protons possessing different isotropic and anisotropic hyperfine couplings were identified. The strength of the hyperfine interaction with one proton suggests a significant covalent O-H binding of carbonyl oxygen O1 that is a characteristic of a neutral radical, an assignment that is also supported by the unusually large hyperfine coupling to the methyl protons. The second proton with a large anisotropic coupling also forms a strong hydrogen bond with a carbonyl oxygen. This second hydrogen bond, which has a significant out-of-plane character, is from an NH2 or NH nitrogen, probably from an arginine (Arg-71) known to be in the quinone binding site. Assignment of the third exchangeable proton with smaller anisotropic coupling is more ambiguous, but it is clearly not involved in a direct hydrogen bond with either of the carbonyl oxygens. The results support a model that the semiquinone is bound to the protein in a very asymmetric manner by two strong hydrogen bonds from Asp-75 and Arg-71 to the O1 carbonyl, while the O4 carbonyl is not hydrogen-bonded to the protein.     

Electron acceptors of bacterial photosynthetic reaction centers II. H+ binding coupled to secondary electron transfer in the quinone acceptor complex

The photoreduction of ubiquinone in the electron acceptor complex (Q₁Q₁₁) of photosynthetic reaction centers from Rhodopseudomonas sphaeroides, R26, was studied in a series of short, saturating flashes. The specific involvement of H⁺ in the reduction was revealed by the pH dependence of the electron transfer events and by net H⁺ binding during the formation of ubiquinol, which requires two turnovers of the photochemical act. On the first flash Q₁₁ receives an electron via Q₁ to form a stable ubisemiquinone anion (Q?^?₁₁); the second flash generates Q?^?₁. At low pH the two semiquinones rapidly disproportionate with the uptake of 2 H⁺, to produce Q₁₁H₂. This yields out-of-phase binary oscillations for the formation of anionic semiquinone and for H⁺ uptake. Above pH 6 there is a progressive increase in H⁺ binding on the first flash and an equivalent decrease in binding on the second flash until, at about pH 9.5, the extent of H⁺ binding is the same on all flashes. The semiquinone oscillations, however, are undiminished up to pH 9. It is suggested that a non-chromophoric, acid-base group undergoes a pK shift in response to the appearance of the anionic semiquinone and that this group is the site of protonation on the first flash. The acid-base group, which may be in the reaction center protein, appears to be subsequently involved in the protonation events leading to fully reduced ubiquinol. The other proton in the two electron reduction of ubiquinone is always taken up on the second flash and is bound directly to Q?^?₁₁. At pH values above 8.0, it is rate limiting for the disproportionation and the kinetics, which are diffusion controlled, are properly responsive to the prevailing pH. Below pH 8, however, a further step in the reaction mechanism was shown to be rate limiting for both H⁺ binding electron transfer following the second flash.     

Electron sweep across four b-hemes of cytochrome bc1 revealed by unusual paramagnetic properties of the Qi semiquinone intermediate

Dimeric cytochromes bc are central components of photosynthetic and respiratory electron transport chains. In their catalytic core, four hemes b connect four quinone (Q) binding sites. Two of these sites, Q_i sites, reduce quinone to quinol (QH₂) in a step-wise reaction, involving a stable semiquinone intermediate (SQ_i). However, the interaction of the SQ_i with the adjacent hemes remains largely unexplored. Here, by revealing the existence of two populations of SQ_i differing in paramagnetic relaxation, we present a new mechanistic insight into this interaction. Benefiting from a clear separation of these SQ_i species in mutants with a changed redox midpoint potential of hemes b, we identified that the fast-relaxing SQ_i (SQ_iF) corresponds to the form magnetically coupled with the oxidized heme b_H (the heme b adjacent to the Q_i site), while the slow-relaxing SQ_i (SQ_iS) reflects the form present alongside the reduced (and diamagnetic) heme b_H. This so far unreported SQ_iF calls for a reinvestigation of the thermodynamic properties of SQ_i and the Q_i site. The existence of SQ_iF in the native enzyme reveals a possibility of an extended electron equilibration within the dimer, involving all four hemes b and both Q_i sites. This substantiates the predicted earlier electron transfer acting to sweep the b-chain of reduced hemes b to diminish generation of reactive oxygen species by cytochrome bc₁. In analogy to the Q_i site, we anticipate that the quinone binding sites in other enzymes may contain yet undetected semiquinones which interact magnetically with oxidized hemes upon progress of catalytic reactions.     

Possible roles of two quinone molecules in direct and indirect proton pumps of bovine heart NADH-quinone oxidoreductase (complex I)

In many energy transducing systems which couple electron and proton transport, for example, bacterial photosynthetic reaction center, cytochrome bc₁-complex (complex III) and E. coli quinol oxidase (cytochrome bo₃ complex), two protein-associated quinone molecules are known to work together. T. Ohnishi and her collaborators reported that two distinct semiquinone species also play important roles in NADH-ubiquinone oxidoreductase (complex I). They were called SQ_Nf (fast relaxing semiquinone) and SQ_Ns (slow relaxing semiquinone). It was proposed that Q_Nf serves as a “direct” proton carrier in the semiquinone-gated proton pump (Ohnishi and Salerno, FEBS Letters 579 (2005) 4555), while Q_Ns works as a converter between one-electron and two-electron transport processes. This communication presents a revised hypothesis in which Q_Nf plays a role in a “direct” redox-driven proton pump, while Q_Ns triggers an “indirect” conformation-driven proton pump. Q_Nf and Q_Ns together serve as (1e^?/2e^?) converter, for the transfer of reducing equivalent to the Q-pool.     

Effect of inhibitors,redox state and isoprenoid chain length on the affinity of ubiquinone for the secondary acceptor binding site in the reaction centers of photosynthetic bacteria

Quinone and inhibitor binding to Rhodopseudomonas sphaeroides (R-26 and GA) reaction centers were studied using spectroscopic methods and by direct adsorption of reaction centers onto anion exchange filters in the presence of ¹⁴C-labelled quinone or inhibitor. These measurements show that as secondary acceptor, Q_B, ubiquinone (UQ) is tightly bound in the semiquinone form and loosely bound in the quinone and quinol forms. The quinol is probably more loosely bound than the quinone. o-Phenanthroline and terbutryn, a triazine inhibitor, compete with UQ and with each other for binding to the reaction center. Inhibition by o-phenanthroline of electron transfer from the primary to the secondary quinone acceptor (Q_A to Q_B) occurs via displacement of UQ from the Q_B binding site. Displacement of UQ by terbutryn is apparently accessory to the inhibition of electron transfer. Terbutryn binding is lowered by reduction of Q_B to Q^?_B but is practically unaffected by reduction of Q_A to Q^?_A in the absence of Q_B. UQ-9 and UQ-10 have a 5- to 6-fold higher binding affinity to the Q_B site than does UQ-1, indicating that the long isoprenoid chain facilitates the binding to the Q_B site.     

The Nitric-oxide Reductase from Paracoccus denitrificans Uses a Single Specific Proton Pathway

The NO reductase from Paracoccus denitrificans reduces NO to N₂O (2NO + 2H⁺ + 2e⁻ → N₂O + H₂O) with electrons donated by periplasmic cytochrome c (cytochrome c-dependent NO reductase; cNOR). cNORs are members of the heme-copper oxidase superfamily of integral membrane proteins, comprising the O₂-reducing, proton-pumping respiratory enzymes. In contrast, although NO reduction is as exergonic as O₂ reduction, there are no protons pumped in cNOR, and in addition, protons needed for NO reduction are derived from the periplasmic solution (no contribution to the electrochemical gradient is made). cNOR thus only needs to transport protons from the periplasm into the active site without the requirement to control the timing of opening and closing (gating) of proton pathways as is needed in a proton pump. Based on the crystal structure of a closely related cNOR and molecular dynamics simulations, several proton transfer pathways were suggested, and in principle, these could all be functional. In this work, we show that residues in one of the suggested pathways (denoted pathway 1) are sensitive to site-directed mutation, whereas residues in the other proposed pathways (pathways 2 and 3) could be exchanged without severe effects on turnover activity with either NO or O₂. We further show that electron transfer during single-turnover reduction of O₂ is limited by proton transfer and can thus be used to study alterations in proton transfer rates. The exchange of residues along pathway 1 showed specific slowing of this proton-coupled electron transfer as well as changes in its pH dependence. Our results indicate that only pathway 1 is used to transfer protons in cNOR.     

Charge polarization imposed by the binding site facilitates enzymatic redox reactions of quinone

Quinone reduction site (Q_i) of cytochrome bc₁ represents one of the canonical sites used to explore the enzymatic redox reactions involving semiquinone (SQ) states. However, the mechanism by which Q_i allows the completion of quinone reduction during the sequential transfers of two electrons from the adjacent heme b_H and two protons to C1- and C4-carbonyl remains unclear. Here we established that the SQ coupled to an oxidized heme b_H is a dominant intermediate of catalytic forward reaction and, contrary to the long-standing assumption, represents a significant population of SQ detected across pH 5–9. The pH dependence of its redox midpoint potential implicated proton exchange with histidine. Complementary quantum mechanical calculations revealed that the SQ anion formed after the first electron transfer undergoes charge and spin polarization imposed by the electrostatic field generated by histidine and the aspartate/lysine pair interacting with the C4- and C1-carbonyl, respectively. This favors a barrierless proton exchange between histidine and the C4-carbonyl, which continues until the second electron reaches the SQ_i. Inversion of charge polarization facilitates the uptake of the second proton by the C1-carbonyl. Based on these findings we developed a comprehensive scheme for electron and proton transfers at Q_i featuring the equilibration between the anionic and neutral states of SQ_i as means for a leak-proof stabilization of the radical intermediate. The key catalytic role of the initial charge/spin polarization of the SQ anion at the active site, inherent to the proposed mechanism, may also be applicable to the other quinone oxidoreductases.     

The lateral diffusion coefficient of lecithin molecules in single bilayer vesicles studied by 14N NMR

The ¹⁴N nuclear relaxation times T₁ and T₂ in egg yolk phosphatidylcholine have been observed in single bilayer vesicles dispersed in the media of different viscosities, ¹H₂O and ²H₂O. The lateral diffusion coefficient of lipid molecule D has been calculated according to the method reported earlier: D = 2.2 × 10^?8cm²s^?1 in ¹H₂O and 2.1 × 10^?8cm²s^?1 in ²H₂O at 20°C. They are in excellent agreement. This result gives a strong basis of usefulness of ¹⁴N NMR method in the evaluation of D without introducing any system perturbation.     

Water binding to the oxygen-evolving system of chloroplasts; effects of isotope substitution on the S2 state EPR spectrum

Replacement of H₂O by ²H₂O in oxygen-evolving Photosystem II preparations caused an increased resolution of the fine structure of the S₂ state EPR spectrum. In both ²H₂O and H₂O samples, comparison of the S₂ spectra generated by illumination at 200 and 283 K (10°C) showed a difference in the fine structure on the hyperfine lines. A reduction in the spacing of the outer hyperfine lines was also observed when samples illuminated at 283 K were compared to those where S₂ was formed by 200 K illumination. The observations are interpreted as due to proton binding, perhaps as water, at or near the manganese complex giving rise to the S₂ signal.     

Self-association of oxyhaemoglobin. A nuclear magnetic relaxation study in H2O/D2O solutions

The proton and deuterium longitudinal relaxation rates were Studied at room temperature up to the highest protein concentrations in oxyhaemoglobin solutions of different H₂O/D₂O composition. The deuterium relaxation rates followed the experimentally well known single linear dependence on protein concentration, the slopes being little influenced by solvent (D₂O/H₂O) composition. The proton ralaxation rates show two different liner dependences on haemoglobin concentration. The entire concentration range is described by two straight lines with the threshold concentration about 11 mM (in haem), The ratio of the slopes is 1.6 (high-to-low Hb-conc.). Only in the higher concentration range two T₁'s were observed if the solvent contained more than half of D₂O. The slow relaxation phase of protons has T₁'s similar to those measured in solutions with less than half of D₂O. The relaxation of the other phase was ten times faster. The ratio of the proton populations in these two phases was equal to 2 (slow-to-fast) and independent of protein concentration. The fast relaxing protons are attributed to water molecules encaged within two or more haemoglobin molecules which associate for times long enough on the PMR time-scale.     

Voltage changes involving photosystem II quinone–iron complex turnover

An electrometrical technique was used to investigate proton-coupled electron transfer between the primary plastoquinone acceptor Q_A⁻ and the oxidized non-heme iron Fe³⁺ on the acceptor side of photosystem II core particles incorporated into phospholipid vesicles. The sign of the transmembrane electric potential difference Δψ (negative charging of the proteoliposome interior) indicates that the iron–quinone complex faces the interior surface of the proteoliposome membrane. Preoxidation of the non-heme iron was achieved by addition of potassium ferricyanide entrapped into proteoliposomes. Besides the fast unresolvable kinetic phase (τ ∼ 0.1 μs) of Δψ generation related to electron transfer between the redox-active tyrosine Y_Z and Q_A, an additional phase in the submillisecond time domain (τ ∼ 0.1 ms at 23°C, pH 7.0) and relative amplitude ∼ 20% of the amplitude of the fast phase was observed under exposure to the first flash. This phase was absent under the second laser flash, as well as upon the first flash in the presence of DCMU, an inhibitor of electron transfer between Q_A and the secondary quinone Q_B. The rate of the additional electrogenic phase is decreased by about one-half in the presence of D₂O and is reduced with the temperature decrease. On the basis of the above observations we suggest that the submillisecond electrogenic reaction induced by the first flash is due to the vectorial transfer of a proton from external aqueous phase to an amino acid residue(s) in the vicinity of the non-heme iron. The possible role of the non-heme iron in cyclic electron transfer in photosystem II complex is discussed.