Proton translocation in chloroplasts and its relationship to electron transport between the photosystems.

Using dark adapted isolated spinach chloroplasts and sequences of brief saturating flashes the correlation of the uptake and release of protons with electron transport from Photosystem II to Photosystem I were studied. The following observations and conclusions are reported: (1) Flash-induced proton uptake shows a weak, damped binary oscillation, with maxima occurring after the 2nd, 4th, etc. flashes. The damping factor is comparable to that observed in the O2 flash yield oscillation and therefore explained by misses in Photosystem II. (2) On the average and after a steady state is reached, each flash (i.e. each reduction of Q) induces the uptake of 2H+ from outside the chloroplasts. (3) Flash induced proton release inside the chloroplast membrane shows a strong damped binary oscillation with maximum release occurring also after the 2nd, 4th, etc. flashes. (4) This phenomenon is correlated with the earlier reported binary oscillations of electron transport [2] and shows that both electrons and protons are transported in pairs between the photosystems. (5) In two sequential flashes 4H+ from the outside of the thylakoid and 2e- from water are accumulated at a binding site B. Subsequently, the two electrons are transferred to non-protonated acceptors in Photosystem I (probably plastocyanin and cytochrome f) and the 4H+ are released inside the thylakoid. (6) It is concluded that a primary proton transporting site and/or energy conserving step located between the photosystems is being observed.     

Stoichiometry of proton release from the catalytic center in photosynthetic water oxidation. Reexamination by a glass electrode study at ph 5.5-7.2.

The catalytic center (CC) of water oxidation in photosystem II passes through four stepwise increased oxidized states (S(0)-S(4)) before O(2) evolution takes place from 2H(2)O in the S(4) --> S(0) transition. The pattern of the release of the four protons from the CC cannot be followed directly in the medium, because proton release from unknown amino acid residues also takes place. However, pH-independent net charge oscillations of 0:0:1:1 in S(0):S(1):S(2):S(3) have been considered as an intrinsic indicator for the H(+) release from the CC. The net charges have been proposed to be created as the charge difference between electron abstraction and H(+) release from the CC. Then the H(+) release from the CC is 1:0:1:2 for the S(0) --> S(1) --> S(2) --> S(3) --> S(0) transition. Strong support for this conclusion is given in this work with the analysis of the pH-dependent pattern of H(+) release in the medium measured directly by a glass electrode between pH 5.5 and 7.2. Improved and crystallizable photosystem II core complexes from the cyanobacterium Synechococcus elongatus were used as material. The pattern can be explained by protons released from the CC with a stoichiometry of 1:0:1:2 and protons from an amino acid group (pK approximately 5.7) that is deprotonated and reprotonated through electrostatic interaction with the oscillating net charges 0:0:1:1 in S(0):S(1):S(2):S(3). Possible water derivatives that circulate through the S states have been named.     

Magnesium ion induced proton release as a probe for the polyelectrolytic structure of ribosomal RNAs and subunits

E coli ribosomes and rRNA's released 20 to 50 protons upon jump of magnesium ion concentration from 1 mM to 20 mM. The Mg2+-induced proton release was measured separately for 16S rRNA, 23S rRNA, 30S subunit, and 50S subunit by a new spectrophotometric method that had a much better sensitivity than the pH-stat method. The proton release from the subunits and rRNA's were similar in the number of protons, the pH dependence that had a minimum at neutral pH, and the upward concaveness of the Scatchard plot. From these results, the main source of protons in ribosomal subunits was assigned to nucleotide bases of rRNA's that showed a downward pKa shift upon Mg2+-ion binding. The subunits and rRNA's, however, differed in the proton release. 16S rRNA released protons somewhat more effectively than 23S rRNA, while 30S subunit released protons 2 to 5 times more effectively than 50S subunit. The marked difference between the two subunits suggest that ionizable bases in 16S and 23S rRNA's are covered and their pKa values are shifted by ribosomal proteins to different extents. The association of 30S and 50S subunits induced little proton release, showing that few ionizable groups with pKa near neutral pH are involved in the association. E. coli tRNA and poly U also showed Mg2+-induced proton release. The amounts of protons released from rRNA's, tRNA, and poly U were roughly proportional to the amount of bases not hydrogen bonded. The Mg2+-induced proton release from the natural and synthetic RNA's can be explained by the electrostatic field effect of polyphosphate backbones on bases not hydrogen bonded, as proposed in a previous paper. It also reflects the conformational structure of each RNA molecule.     

Time-resolved infrared detection of the proton and protein dynamics during photosynthetic oxygen evolution

Photosynthetic oxygen evolution by plants and cyanobacteria is performed by water oxidation at the Mn(4)CaO(5) cluster in photosystem II. The reaction is known to proceed via a light-driven cycle of five intermediates called S(i) states (i = 0-4). However, the detailed reaction processes during the intermediate transitions remain unresolved. In this study, we have directly detected the proton and protein dynamics during the oxygen-evolving reactions using time-resolved infrared spectroscopy. The time courses of the absorption changes at 1400 and 2500 cm(-1), which represent the reactions and/or interaction changes of carboxylate groups and the changes in proton polarizability of strong hydrogen bonds, respectively, were monitored upon flash illumination. The results provided experimental evidence that during the S(3) → S(0) transition, drastic proton rearrangement, most likely reflecting the release of a proton from the catalytic site, takes place to form a transient state before the oxidation of the Mn(4)CaO(5) cluster that leads to O(2) formation. Early proton movement was also detected during the S(2) → S(3) transition. These observations reveal the common mechanism in which proton release facilitates the transfer of an electron from the Mn(4)CaO(5) cluster in the S(2) and S(3) states that already accumulate oxidizing equivalents. In addition, relatively slow rearrangement of carboxylate groups was detected in the S(0) → S(1) transition, which could contribute to the stabilization of the S(1) state. This study demonstrates that time-resolved infrared detection is a powerful method for elucidating the detailed molecular mechanism of photosynthetic oxygen evolution by pursuing the reactions of substrate and amino acid residues during the S-state transitions.     

Proton release during the four steps of photosynthetic water oxidation: induction of 1:1:1:1 pattern due to lack of chlorophyll a/b binding proteins.

In photosynthesis of green plants water is oxidized to dioxygen. This four-step process is accompanied by the release of four protons (per molecule of dioxygen) into the lumen of thylakoids. In dark-adapted thylakoids which are excited with a series of short flashes of light, the extent of proton release oscillates with period four as a function of flash number. Noninteger and pH-dependent proton/electron ratios (e.g., 1.1, 0.25, 1.0, and 1.65 at pH 7) have been attributed to a superposition of two reactions: chemical production of protons and transient electrostatic response of peripheral amino acid side chains. Aiming at the true pattern of proton production, we investigated the relative contribution of peripheral proteins. Thylakoids with and without chlorophyll a/b binding proteins were compared. Thylakoids lacking chlorophyll a/b binding proteins were prepared from pea seedlings grown under intermittent light [Jahns, P., & Junge, W. (1992) Biochemistry (preceding paper in this issue)]. We found no oscillation of proton release in the pH range from 6 to 7.5. These and other results showed that chlorophyll a/b binding proteins, which primarily serve as light-harvesting antennas, modulate proton release by water oxidation. A nonoscillating pattern of proton release, with proton/electron ratios of 1:1:1:1 more closely represents the events in the catalytic center proper. This implies hydrogen abstraction rather than electron abstraction from water during the oxygen-evolving step S3----S0.     

Mg2+-induced proton release from Escherichia coli ribosome and ribosomal RNA

Escherichia coli ribosome released protons upon addition of Mg2+. The Mg2+-induced proton release was studied by means of the pH-stat technique. The number of protons released from a 70 S ribosome in the Mg2+ concentration range 1-20 mM was about 30 at pH 7 and 7.6, and increased to about 40 at pH 6.5. The rRNA mixture extracted from 70 S ribosome showed proton release of amount and of pH dependence similar to those of the 70 S ribosome but the ribosomal protein mixture released few. This indicates that rRNA is the main source of the protons released from ribosome. The pH titration of rRNA showed that the pKa values of nucleotide bases were downward shifted upon Mg2+ binding. This pKa shift can account for the proton release. The Scatchard plots of proton release from rRNA and ribosome were concave upward, showing that the Mg2+-binding sites leading to proton release were either heterogeneous or had a negative cooperativity. A model assuming heterogeneous Mg2+-binding sites is shown to be unable to explain the proton release. Electrostatic field effect models are proposed in which Mg2+ modulates the electrostatic field of phosphate groups and the potential change induces a shift of the pKa values of bases that leads to the proton release. These models can explain the main features of the proton release.     

Electrostatics and proton transfer in photosynthetic water oxidation

Photosystem II (PSII) oxidizes two water molecules to yield dioxygen plus four protons. Dioxygen is released during the last out of four sequential oxidation steps of the catalytic centre (S(0) --> S(1), S(1) --> S(2), S(2) --> S(3), S(3) --> S(4) --> S(0)). The release of the chemically produced protons is blurred by transient, highly variable and electrostatically triggered proton transfer at the periphery (Bohr effect). The extent of the latter transiently amounts to more than one H(+)/e(-) under certain conditions and this is understood in terms of electrostatics. By kinetic analyses of electron-proton transfer and electrochromism, we discriminated between Bohr-effect and chemically produced protons and arrived at a distribution of the latter over the oxidation steps of 1 : 0 : 1 : 2. During the oxidation of tyr-161 on subunit D1 (Y(Z)), its phenolic proton is not normally released into the bulk. Instead, it is shared with and confined in a hydrogen-bonded cluster. This notion is difficult to reconcile with proposed mechanisms where Y(Z) acts as a hydrogen acceptor for bound water. Only in manganese (Mn) depleted PSII is the proton released into the bulk and this changes the rate of electron transfer between Y(Z) and the primary donor of PSII P(+)(680) from electron to proton controlled. D1-His190, the proposed centre of the hydrogen-bonded cluster around Y(Z), is probably further remote from Y(Z) than previously thought, because substitution of D1-Glu189, its direct neighbour, by Gln, Arg or Lys is without effect on the electron transfer from Y(Z) to P(+)(680) (in nanoseconds) and from the Mn cluster to Y(ox)(Z).     

FTIR detection of water reactions in the oxygen-evolving centre of photosystem II

Flash-induced Fourier transform infrared (FTIR) difference spectroscopy has been used to study the water-oxidizing reactions in the oxygen-evolving centre of photosystem II. Reactions of water molecules were directly monitored by detecting the OH stretching bands of weakly H-bonded OH of water in the 3700-3500 cm(-1) region in FTIR difference spectra during S-state cycling. In the S1-->S2 transition, a band shift from 3588 to 3617 cm(-1) was observed, indicative of a weakened H-bond. Decoupling experiments using D2O:H2O (1:1) showed that this OH arose from a water molecule with an asymmetric H-bonding structure and this asymmetry became more significant upon S2 formation. In the S2-->S3, S3-->S0 and S0-->S1 transitions, negative bands were observed at 3634, 3621 and 3612 cm(-1), respectively, representing formation of a strong H-bond or a proton release reaction. In addition, using complex spectral features in the carboxylate stretching region (1600-1300 cm-(1)) as 'fingerprints' of individual S-state transitions, pH dependency of the transition efficiencies and the effect of dehydration were examined to obtain the information of proton release and water insertion steps in the S-state cycle. Low-pH inhibition of the S2-->S3, S3-->S0 and S0-->S1 transitions was consistent with a view that protons are released in the three transitions other than S1-->S2, while relatively high susceptibility to dehydration in the S2-->S3 and S3-->S0 transitions suggested the insertion of substrate water into the system during these transitions. Thus, a possible mechanism of water oxidation to explain the FTIR data is proposed.     

ATP-synthase of Rhodobacter capsulatus: coupling of proton flow through F0 to reactions in F1 under the ATP synthesis and slip conditions

A stepwise increasing membrane potential was generated in chromatophores of the phototrophic bacterium Rhodobacter capsulatus by illumination with short flashes of light. Proton transfer through ATP-synthase (measured by electrochromic carotenoid bandshift and by pH-indicators) and ATP release (measured by luminescence of luciferin-luciferase) were monitored. The ratio between the amount of protons translocated by F0F1 and the ATP yield decreased with the flash number from an apparent value of 13 after the first flash to about 5 when averaged over three flashes. In the absence of ADP, protons slipped through F0F1. The proton transfer through F0F1 after the first flash contained two kinetic components, of about 6 ms and 20 ms both under the ATP synthesis conditions and under slip. The slower component of proton transfer was substantially suppressed in the absence of ADP. We attribute our observations to the mechanism of energy storage in the ATP-synthase needed to couple the transfer of four protons with the synthesis of one molecule of ATP. Most probably, the transfer of initial protons of each tetrad creates a strain in the enzyme that slows the translocation of the following protons.     

Electron transfer and proton pumping under excitation of dark-adapted chloroplasts with flashes of light

Proton release inside thylakoids, which is linked to the action of the water-oxidizing enzyme system, was investigated spectrophotometrically with the dye neutral red under conditions when the external phase was buffered. Under excitation of dark-adapted chloroplasts with four short laser flashes in series, the pattern of proton release as a function of the flash number was recorded and interpreted in the light of the generally accepted scheme for consecutive transitions of the water-oxidizing enzyme system: S₀ → S₁, S₁ → S₂, S₂ → S₃, S₃ → S₄, S₀. It was found that the proton yield after the first flash varied in a reproducible manner, being dependent upon the dark pretreatment given. In terms of the proton-electron reaction during these transitions, the pattern was as follows. In strictly dark-adapted chloroplasts (frozen chloroplasts thawed in darkness and kept for at least 7 min in the dark after dilution), it was fitted well by a stoichiometry of 1:0:1:2. In a less stringently dark-adapted preparation (as above but thawed under light), it was fitted by 0:1:1:2. Mechanistically this is not yet understood. However, it is a first step towards resolving controversy over this pattern among different laboratories. Under conditions where the 1:0:1:2 stoichiometry was observed, proton release was time resolved. Components with half-rise times of 500 and 1000 μs could be correlated with the S₂ → S₃ and S₃ → S₄ transitions, respectively. Proton release during the S₀ → S₁ transition is more rapid, but is less well attributable to the transitions due to error proliferation. A distinct component with a half-rise time of only 100 μs was observed after the second flash. Since it did not fit into the expected kinetics (based on literature data) for the S_i → S_i+1 transitions, we propose that it reflects proton release from a site which is closer to the reaction center of Photosystem (PS) II than the water-splitting enzyme system. This is supported by the observation of rapid proton release under conditions where water oxidation is blocked. Related experiments on the pattern of proton uptake at the reducing side of PS II indicated that protons act as specific counterions for semiquinone anions without binding to them.     

S-state dependent Fourier transform infrared difference spectra for the photosystem II oxygen evolving complex

Vibrational spectroscopy provides a means to investigate molecular interactions within the active site of an enzyme. We have applied difference FTIR spectroscopy coupled with a flash turnover protocol of photosystem II (PSII) to study the oxygen evolving complex (OEC). Our data show two overlapping oscillatory patterns as the sample is flashed through the four-step S-state cycle that produces O(2) from two H(2)O molecules. The first oscillation pattern of the spectra shows a four-flash period four oscillation and reveals a number of new vibrational modes for each S-state transition, indicative of unique structural changes involved in the formation of each S-state. Importantly, the first and second flash difference spectra are reproduced in the 1800-1200 cm(-)(1) spectral region by the fifth and sixth flash difference spectra, respectively. The second oscillation pattern observed is a four-flash, period-two oscillation associated with changes primarily to the amide I and II modes and reports on changes in sign of these modes that alternate 0:0:1:1 during S-state advance. This four-flash, period-two oscillation undergoes sign inversion that alternates during the S(1)-to-S(2) and S(3)-to-S(0) transitions. Underlying this four-flash period two is a small-scale change in protein secondary structure in the PSII complex that is directly related to S-state advance. These oscillation patterns and their relationships with other PSII phenomena are discussed, and future work can initiate more detailed vibrational FTIR studies for the S-state transitions providing spectral assignments and further structural and mechanistic insight into the photosynthetic water oxidation reaction.     

Effects of removal and reconstitution of the extrinsic 33, 24 and 16 kDa proteins on flash oxygen yield in Photosystem II particles

The effects of removal and reconstitution of the three extrinsic proteins on the flash O₂ yield were investigated and the following results were obtained. (1) Removal in darkness of the 24 and 16 kDa proteins affected neither the oscillation pattern nor the signal amplitude of the flash O₂ yield. However, the signal amplitude was reduced with a factor of 2 in the presence of EDTA and was restored by excess Ca²⁺. The EDTA treatment did not change the oscillation pattern of the flash O₂ yield, but considerably damped the oscillation pattern of thermoluminescence B band. These results suggest a heterogeneity among the centers in binding affinity for Ca²⁺, and that Ca²⁺ removal induces an all-or-none type inactivation of O₂ evolution but not in the thermoluminescence processes, indicative of an inhibition of the S-state turnover at a specific S-state. (2) Removal in darkness of the 33, 24 and 16 kDa proteins abolished the flash O₂ yield, but the inhibited yield was appreciably restored either by reconstitution with the 33 kDa protein or by inclusion of 200 mM Cl⁻ in the reaction mixture. The flash O₂ yield reconstituted by the 33 kDa protein exhibited a rather normal oscillation pattern accompanied by a slightly increased damping, which could be simulated by assuming a high miss factor (30%) for S₃ → S₀ transition. The Cl⁻-restored flash O₂ yield exhibited a strongly damped oscillation pattern with obscured maxima at the 4th and 8th flashes, which was simulated by assuming a much higher miss factor (70%) for S₃ → S₀ transition. It was indicated that the Cl⁻-restored O₂ evolution considerably differs from the 33 kDa protein-reconstituted O₂ evolution with respect to the mechanism of S-state turnover.     

An investigation of heavy meromyosin-ADP binding equilibria by proton release measurements.

The interaction of magnesium-ADP with skeletal muscle heavy meromyosin has been studied by measuring the accompanying release of protons. Total pH changes of the order of 0.03 were involved, and measurements were performed with a discrimination of some ten-thousandths of a pH unit. At pH 8.0 and 25 degrees C about 0.5 mol of protons per mol of heavy meromyosin is released at saturation. A stoichiometry of binding close to 2 mol of ADP per mol of protein was found, with a binding constant, obtained from the proton release titration curve (pH 8.0, 25 degrees C), of 2 X 10(5) M-1. At 5 degrees C the release of protons per mole is slightly greater, and the binding constant is somewhat increased, reflecting a negative enthalpy of binding. Similar proton release behavior is observed in the presence of manganous ions in place of magnesium. The liberation of protons is thus unrelated to the temperature-dependent isomerization of myosin in the presence of substrate. Alkylation of a reactive thiol group (SH1) does not change the proton liberation at pH 8.0. From the pH dependence of proton release, the association constant of heavy meromyosin with magnesium-ADP at other pH values can be inferred and shows an appreciable rise as the pH increases. The pH-proton release profile also allows the pK of the ionizing groups perturbed by the ligand to be deduced. At least two groups ionizing above pH 7 and one below are involved. Their pK's in the unperturbed state are assigned as 8.5, 9.3, and about 6.6, respectively; they are displaced in the complex to about 8.0, 9.1, and 6.3. A relation to the pH-activity profile of myosin ATPase is indicated. The pH-proton release profile is somewhat changed when the SH1 group is alkylated. Measurements with potassium-ADP, in the absence of magnesium, show that at pH 8.0 there is no proton release but rather a sizeable proton absorption (about 0.5 mol of protons per mol of heavy meromyosin). The association constant derived from the titration curves (pH 8.0, 25 degrees C) is 3 X 10(4) M-1.     

pH dependence of the multiline, manganese EPR signal for the 'S2' state in PS II particles. Absence of proton release during the S1----S2 electron transfer step of the oxygen evolving system

The pH dependence of oxygen evolution rates, 2,6-dichlorophenolindophenol (DCIP) reduction rates and the intensity of the multiline manganese EPR signal associated with the S2K ok state has been studied using oxygen-evolving spinach (PS) II particles. The oxygen evolution and DCIP reduction rates are found to be very sensitive to pH, with the maximal rates occurring at pH 6.5-7.0. Both the rate and yield of the S2 multiline manganese EPR signal intensity, produced by single flash excitation at room temperature or by continuous illumination at 200 K, are found to be independent of pH, indicating that no proton is released from this manganese site during the S1----S2 electron transfer. These results agree with those from other laboratories showing no proton release on this transition, but using techniques monitoring other species.     

The onset of the deuterium isotope effect in cytochrome c oxidase

We have investigated the dynamics of proton equilibration within the proton-transfer pathway of cytochrome c oxidase from bovine heart that is used for the transfer of both substrate and pumped protons during reaction of the reduced enzyme with oxygen (D-pathway). The kinetics of the slowest phase in the oxidation of the enzyme (the oxo-ferryl --> oxidized transition, F --> O), which is associated with proton uptake, were studied by monitoring absorbance changes at 445 nm. The rate constant of this transition, which is 800 s(-)(1) in H(2)O (at pH approximately 7.5), displayed a kinetic deuterium isotope effect of approximately 4 (i.e., the rate was approximately 200 s(-)(1) in 100% D(2)O). To investigate the kinetics of the onset of the deuterium isotope effect, fully reduced, solubilized CO-bound cytochrome c oxidase in H(2)O was mixed rapidly at a ratio of 1:5 with a D(2)O buffer saturated with oxygen. After a well-defined time period, CO was flashed off using a short laser flash. The time between mixing and flashing off CO was varied within the range 0. 04-10 s. The results show that for the bovine enzyme, the onset of the deuterium isotope effect takes place within two time windows of O transition is internal proton transfer from a site, proposed to be Glu (I-286) (R. sphaeroides amino acid residue numbering), to the binuclear center. The spontaneous equilibration of protons/deuterons with this site in the interior of the protein is slow (approximately 1 s).     

Determination of H+/e- ratios in chloroplasts with flashing light.

Using a rapid pH electrode, measurements were made of the flash-induced proton transport in isolated spinach chloroplasts. To calibrate the system, we assumed that in the presence of ferricyanide and in steady-state flashing light, each flash liberates from water one proton per reaction chain. We concluded that with both ferricyanide and methylviologen as acceptors two protons per electron are translocated by the electron transport chain connecting Photosystem II and I. With methyl viologen but not with ferricyanide as an acceptor, two additional protons per electron are taken up due to Photosystem I activity. One of these latter protons is translocated to the inside of the thylakoid while the other is taken up in H2O2 formation. Assuming that the proton released during water splitting remains inside the thylakoid, we compute H+/e- ratios of 3 and 4 for ferricyanide and methylviologen, respectively. In continuous light of low intensity, we obtained the same H+/e- ratios. However, with higher intensities where electron transport becomes rate limited by the internal pH, the H+/e- ratio approached 2 as a limit for both acceptors. A working model is presented which includes two sites of proton translocation, one between the photoacts, the other connected to Photosystem I, each of which translocates two protons per electron. Each site presents a approximately 30 ms diffusion barrier to proton passage which can be lowered by uncouplers to 6-10 ms.     

Proton concentration jumps and generation of transmembrane pH-gradients by photolysis of 4-formyl-6-methoxy-3-nitrophenoxyacetic acid

Proton concentration gradients across membranes are important for many biological energy transducing processes. The kinetics of proton dependent processes can be studied by pH-jump methods in which protons are photochemically released. In the following we describe the synthesis and the properties of photolabile 4-formyl-6-methoxy-3-nitrophenoxyacetic acid, a 'caged proton'. The synthesis is based on vanillin, which is alkylated with chloroacetic acid to give a carboxylic acid (pK = 2.72). In a second step a nitro group ortho to the formyl group is introduced. Photochemical proton release occurs by a reaction mechanism analogous to the well known photochemical formation of 2-nitrosobenzoic acid from 2-nitrobenzaldehyde. The pK values of the photoproduct are 0.75 and 2.76, respectively, thus allowing the use of the compound in a wide pH-range. The quantum yield is 0.18, lower than in the case of the 2-nitrobenzaldehyde/2-nitrosobenzoic acid system (phi = 0.5). The release of the proton in a flash photolysis experiment occurs within less than 1 microseconds. The spectrum of photolabile compound has absorption maxima at 263 nm and 345 nm, respectively. Its permeability across a lipid bilayer membrane is very low (permeability coefficient Pd approximately equal to 10(-9) cm.s-1 at pH 8) so that transmembrane proton concentration gradients can be generated.     

pH dependence of proton translocation in the oxidative and reductive phases of the catalytic cycle of cytochrome c oxidase. The role of H2O produced at the oxygen-reduction site

A study is presented on the pH dependence of proton translocation in the oxidative and reductive phases of the catalytic cycle of purified cytochrome c oxidase (COX) from beef heart reconstituted in phospholipid vesicles (COV). Protons were shown to be released from COV both in the oxidative and reductive phases. In the oxidation by O2 of the fully reduced oxidase, the H+/COX ratio for proton release from COV (R --> O transition) decreased from approximately 2.4 at pH 6.5 to approximately 1.8 at pH 8.5. In the direct reduction of the fully oxidized enzyme (O --> R transition), the H+/COX ratio for proton release from COV increased from approximately 0.3 at pH 6.5 to approximately 1.6 at pH 8.5. Anaerobic oxidation by ferricyanide of the fully reduced oxidase, reconstituted in COV or in the soluble case, resulted in H+ release which exhibited, in both cases, an H+/COX ratio of 1.7-1.9 in the pH range 6.5-8.5. This H+ release associated with ferricyanide oxidation of the oxidase, in the absence of oxygen, originates evidently from deprotonation of acidic groups in the enzyme cooperatively linked to the redox state of the metal centers (redox Bohr protons). The additional H+ release (O2 versus ferricyanide oxidation) approaching 1 H+/COX at pH < or = 6.5 is associated with the reduction of O2 by the reduced metal centers. At pH > or = 8.5, this additional proton release takes place in the reductive phase of the catalytic cycle of the oxidase. The H+/COX ratio for proton release from COV in the overall catalytic cycle, oxidation by O2 of the fully reduced oxidase directly followed by re-reduction (R --> O --> R transition), exhibited a bell-shaped pH dependence approaching 4 at pH 7.2. A mechanism for the involvement in the proton pump of the oxidase of H+/e- cooperative coupling at the metal centers (redox Bohr effects) and protonmotive steps of reduction of O2 to H2O is presented.