The effect of pH on redox titrations of haem a in cyanide-liganded cytochrome-c oxidase: experimental and modelling studies

High stability of the radical at the catalytic center of cytochrome c oxidase

In aerobic organisms, cellular respiration is associated with electron transfer through a respiratory system of membrane-bound complexes. This electron flow is terminated by the reduction of dioxygen to water by respiratory oxidases. Cytochrome c oxidase (CcO) is a widely distributed heme-copper-oxygen reductase (HCO) found in all mitochondria and some bacteria. However, the sequential reduction of O2 to water in CcO generates a protein-based radical at the catalytic heme a3-CuB site. To avoid the potential damage from the radical, CcO has apparently developed protective mechanisms. Protection by transfer of the highly oxidizing equivalent over considerable distances away from the catalytic site by redox-active Tyr/Trp chains has been previously demonstrated in bovine CcO. However, the rate of the radical migration from the catalytic center has not yet been determined for any HCO. In this work, we show that the radical escapes from the catalytic center of the ferryl PM intermediate of bovine CcO within minutes, which is much longer than the time of its functional reduction during cellular respiration. Apparently, this high stability has evolved to avoid the dissipation of energy released during the oxygen reduction with substrate electrons.

Examination of 'high-energy' metastable state of the oxidized (OH) bovine cytochrome c oxidase: Proton uptake and reaction with H2O2

Reoxidized cytochrome c oxidase appears to be in a 'high-energy' metastable state (OH) in which part of the energy released in the redox reactions is stored. The OH is supposed to relax to the resting 'as purified' oxidized state (O) in a time exceeding 200 ms. The catalytic heme a3-CuB center of these two forms should differ in a protonation and ligation state and the transition of OH-to-O is suggested to be associated with a proton transfer into this center. Employing a stopped-flow and UV-Vis absorption spectroscopy we investigated a proton uptake during the predicted relaxation of OH. It is shown, using a pH indicator phenol red, that from the time when the oxidation of the fully reduced CcO is completed (∼25 ms) up to ∼10 min, there is no uptake of a proton from the external medium (pH 7.8). Moreover, interactions of the assumed OH, generated 100 ms after oxidation of the fully reduced CcO, and the O with H2O2 (1 mM), result in the formation of two ferryl intermediates of the catalytic center, P and F, with very similar kinetics and the amounts of the formed ferryl states in both cases. These results implicate that the relaxation time of the catalytic center during the OH-to-O transition is either shorter than 100 ms or there is no difference in the structure of heme a3-CuB center of these two forms.

Electron Transfer Coupled to Conformational Dynamics in Cell Respiration

Cellular respiration is a fundamental process required for energy production in many organisms. The terminal electron transfer complex in mitochondrial and many bacterial respiratory chains is cytochrome c oxidase (CcO). This converts the energy released in the cytochrome c/oxygen redox reaction into a transmembrane proton electrochemical gradient that is used subsequently to power ATP synthesis. Despite detailed knowledge of electron and proton transfer paths, a central question remains as to whether the coupling between electron and proton transfer in mammalian mitochondrial forms of CcO is mechanistically equivalent to its bacterial counterparts. Here, we focus on the conserved span between H376 and G384 of transmembrane helix (TMH) X of subunit I. This conformationally-dynamic section has been suggested to link the redox activity with the putative H pathway of proton transfer in mammalian CcO. The two helix X mutants, Val380Met (V380M) and Gly384Asp (G384D), generated in the genetically-tractable yeast CcO, resulted in a respiratory-deficient phenotype caused by the inhibition of intra-protein electron transfer and CcO turnover. Molecular aspects of these variants were studied by long timescale atomistic molecular dynamics simulations performed on wild-type and mutant bovine and yeast CcOs. We identified redox- and mutation-state dependent conformational changes in this span of TMH X of bovine and yeast CcOs which strongly suggests that this dynamic module plays a key role in optimizing intra-protein electron transfers.

Modulation of the electron-proton coupling at cytochrome a by the ligation of the oxidized catalytic center in bovine cytochrome c oxidase

Cytochrome a was suggested as the key redox center in the proton pumping process of bovine cytochrome c oxidase (CcO). Recent studies showed that both the structure of heme a and its immediate vicinity are sensitive to the ligation and the redox state of the distant catalytic center composed of iron of cytochrome a₃ (Fe_a3) and copper (Cu_B). Here, the influence of the ligation at the oxidized Fe_a3³⁺-Cu_B²⁺ center on the electron-proton coupling at heme a was examined in the wide pH range (6.5-11). The strength of the coupling was evaluated by the determination of pH dependence of the midpoint potential of heme a (E_m(a)) for the cyanide (the low-spin Fe_a3³⁺) and the formate-ligated CcO (the high-spin Fe_a3³⁺). The measurements were performed under experimental conditions when other three redox centers of CcO are oxidized. Two slightly differing linear pH dependencies of E_m(a) were found for the CN- and the formate-ligated CcO with slopes of -13 mV/pH unit and -23 mV/pH unit, respectively. These linear dependencies indicate only a weak and unspecific electron-proton coupling at cytochrome a in both forms of CcO. The lack of the strong electron-proton coupling at the physiological pH values is also substantiated by the UV-Vis absorption and electron-paramagnetic resonance spectroscopy investigations of the cyanide-ligated oxidized CcO. It is shown that the ligand exchange at Fe_a³⁺ between His-Fe_a³⁺-His and His-Fe_a³⁺-OH^- occurs only at pH above 9.5 with the estimated pK >11.0.

The H channel is not a proton transfer path in yeast cytochrome c oxidase

Cytochrome c oxidases (CcOs) in the respiratory chains of mitochondria and bacteria are primary consumers of molecular oxygen, converting it to water with the concomitant pumping of protons across the membrane to establish a proton electrochemical gradient. Despite a relatively well understood proton pumping mechanism of bacterial CcOs, the role of the H channel in mitochondrial forms of CcO remains debated. Here, we used site-directed mutagenesis to modify a central residue of the lower span of the H channel, Q413, in the genetically tractable yeast Saccharomyces cerevisiae. Exchange of Q413 to several different amino acids showed no effect on rates and efficiencies of respiratory cell growth, and redox potential measurements indicated minimal electrostatic interaction between the 413 locus and the nearest redox active component heme a. These findings clearly exclude a primary role of this section of the H channel in proton pumping in yeast CcO. In agreement with the experimental data, atomistic molecular dynamics simulations and continuum electrostatic calculations on wildtype and mutant yeast CcOs highlight potential bottlenecks in proton transfer through this route. Our data highlight the preference for neutral residues in the 413 locus, precluding sufficient hydration for formation of a proton conducting wire.

Spectral components of detergent-solubilized bovine cytochrome oxidase

Cytochrome oxidase is the terminal oxidase of the mitochondrial electron transport chain and pumps 4 protons per oxygen reduced to water. Spectral shifts in the α-band of heme a have been observed in multiple studies and these shifts have the potential to shed light on the proton pumping intermediates. Previously we found that heme a had two spectral components in the α-band during redox titrations in living RAW 264.7 mouse macrophage cells, the classical 605 nm form and a blue-shifted 602 nm form. To confirm these spectral changes were not an artifact due to the complex milieu of the living cell, redox titrations were performed in the isolated detergent-solubilized bovine enzyme from both the Soret- and α-band using precise multiwavelength spectroscopy. This data verified the presence of the 602 nm form in the α-band, revealed a similar shift of heme a in the Soret-band and ruled out the reversal of calcium binding as the origin of the blue shift. The 602 nm form was found to be stabilized at high pH or by binding of azide, which is known to blue shift the α-band of heme a. Azide also stabilized the 602 nm form in the living cells. It is concluded there is a form of cytochrome oxidase in which heme a undergoes a blue shift to a 602 nm form and that redox titrations can be successfully performed in living cells where the oxidase operates in its authentic environment and in the presence of a proton motive force.

Effect of Ca2+ on the redox potential of heme a in cytochrome c oxidase

Subunit I of cytochrome c oxidase (CcO) from mitochondria and many bacteria contains a cation binding site (CBS) located at the outer positively charged aqueous phase not far from heme a. Binding of Ca²⁺ with the CBS in bovine CcO inhibits activity of the enzyme 2-3 -fold [Vygodina, T., Kirichenko, A. & Konstantinov A.A. (2013) Direct Regulation of Cytochrome c Oxidase by Calcium Ions, PLoS One.8 e74436]. Here we show that binding of Ca²⁺ at CBS of bovine CcO shifts E_m of heme a to the positive by 15-20 mV. Na⁺ ions that bind to the same site and compete with Ca²⁺ do not affect E_m of heme a and also prevent and reverse the effect of Ca²⁺. No effect of Ca²⁺ or EGTA is observed on E_m of heme a with the wild type bacterial oxidases from R.sphaeroides or P.denitrificans that contain tightly-bound calcium at the site. In the D477A mutant CcO from P. denitrificans that binds Ca²⁺ reversibly like the mitochondrial CcO, calcium shifts redox titration curve of heme a to the positive by ∼35-50 mV that is in good agreement with the results of electrostatic calculations; however, as shown earlier, it does not inhibit CcO activity of the mutant enzyme. Therefore the data do not support the proposal that the inhibitory effect of Ca²⁺ on CcO activity may be explained by the Ca²⁺-induced shift of E_m of heme a. Rather, Ca²⁺ retards electron transfer by inhibition of charge dislocation in the exit part of the proton channel H in mammalian CcO, that is absent in the bacterial oxidases.

Insights into functions of the H channel of cytochrome c oxidase from atomistic molecular dynamics simulations

Proton pumping A-type cytochrome c oxidase (CcO) terminates the respiratory chains of mitochondria and many bacteria. Three possible proton transfer pathways (D, K, and H channels) have been identified based on structural, functional, and mutational data. Whereas the D channel provides the route for all pumped protons in bacterial A-type CcOs, studies of bovine mitochondrial CcO have led to suggestions that its H channel instead provides this route. Here, we have studied H-channel function by performing atomistic molecular dynamics simulations on the entire, as well as core, structure of bovine CcO in a lipid-solvent environment. The majority of residues in the H channel do not undergo large conformational fluctuations. Its upper and middle regions have adequate hydration and H-bonding residues to form potential proton-conducting channels, and Asp51 exhibits conformational fluctuations that have been observed crystallographically. In contrast, throughout the simulations, we do not observe transient water networks that could support proton transfer from the N phase toward heme a via neutral His413, regardless of a labile H bond between Ser382 and the hydroxyethylfarnesyl group of heme a In fact, the region around His413 only became sufficiently hydrated when His413 was fixed in its protonated imidazolium state, but its calculated pK_a is too low for this to provide the means to create a proton transfer pathway. Our simulations show that the electric dipole moment of residues around heme a changes with the redox state, hence suggesting that the H channel could play a more general role as a dielectric well.

The unusual redox properties of C-type oxidases

Cytochrome cbb₃ (also known as C-type) oxidases belong to the family of heme-copper terminal oxidases which couple at the end of the respiratory chain the reduction of molecular oxygen into water and the pumping of protons across the membrane. They are expressed most often at low pressure of O₂ and they exhibit a low homology of sequence with the cytochrome aa₃ (A-type) oxidases found in mitochondria. Their binuclear active site comprises a high-spin heme b₃ associated with a Cu_B center. The protein also contains one low-spin heme b and 3 hemes c. We address here the redox properties of cbb₃ oxidases from three organisms, Rhodobacter sphaeroides, Vibrio cholerae and Pseudomonas stutzeri by means of electrochemical and spectroscopic techniques. We show that the redox potential of the heme b₃ exhibits a relatively low midpoint potential, as in related cytochrome c-dependent nitric oxide reductases. Potential implications for the coupled electron transfer and proton uptake mechanism of C-type oxidases are discussed.

Re-evaluation of the near infrared spectra of mitochondrial cytochrome c oxidase: Implications for non invasive in vivo monitoring of tissues

We re-determined the near infrared (NIR) spectral signatures (650–980 nm) of the different cytochrome c oxidase redox centres, in the process separating them into their component species. We confirm that the primary contributor to the oxidase NIR spectrum between 700 and 980 nm is cupric Cu_A, which in the beef heart enzyme has a maximum at 835 nm. The 655 nm band characterises the fully oxidised haem a₃/Cu_B binuclear centre; it is bleached either when one or more electrons are added to the binuclear centre or when the latter is modified by ligands. The resulting ‘perturbed’ binuclear centre is also characterised by a previously unreported broad 715–920 nm band. The NIR spectra of certain stable liganded species (formate and CO), and the unstable oxygen reaction compounds P and F, are similar, suggesting that the latter may resemble the stable species electronically. Oxidoreduction of haem a makes no contribution either to the 835 nm maximum or the 715 nm band. Our results confirm the ability of NIRS to monitor the Cu_A centre of cytochrome oxidase activity in vivo, although noting some difficulties in precise quantitative interpretations in the presence of perturbations of the haem a₃/Cu_B binuclear centre.

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The NIR spectrum of cytochrome oxidase was deconvoluted into its component species.

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The dominant feature between 700 and 980 nm was confirmed as the CuA chromophore.

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There was no significant contribution from the haem a iron centre.

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A new feature between 715 and 920 nm was assigned to the haem a₃/Cu_B binuclear centre.

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Changes in concentrations of oxygen intermediates P and F may be measurable in vivo.

IR signatures of the metal centres of bovine cytochrome c oxidase: assignments and redox-linkage

Assignments of IR bands of reduced minus oxidized IR difference spectra of bovine and related cytochrome c oxidases are reviewed and their linkages to specific metal centres are assessed. To aid this, redox-poised difference spectra in the presence of cyanide or carbon monoxide are presented. These ligands fix the redox states of either haem a3 alone or haem a3 and CuB respectively, while allowing redox cycling of the remaining centres.

Functions of the hydrophilic channels in protonmotive cytochrome c oxidase

The structures and functions of hydrophilic channels in electron-transferring membrane proteins are discussed. A distinction is made between proton channels that can conduct protons and dielectric channels that are non-conducting but can dielectrically polarize in response to the introduction of charge changes in buried functional centres. Functions of the K, D and H channels found in A1-type cytochrome c oxidases are reviewed in relation to these ideas. Possible control of function by dielectric channels and their evolutionary relation to proton channels is explored.

Coupled electron and proton transfer reactions during the O→E transition in bovine cytochrome c oxidase

A combined DFT/electrostatic approach is employed to study the coupling of proton and electron transfer reactions in cytochrome c oxidase (CcO) and its proton pumping mechanism. The coupling of the chemical proton to the internal electron transfer within the binuclear center is examined for the O→E transition. The novel features of the His291 pumping model are proposed, which involve timely well-synchronized sequence of the proton-coupled electron transfer reactions. The obtained pK(a)s and E(m)s of the key ionizable and redox-active groups at the different stages of the O→E transition are consistent with available experimental data. The PT step from E242 to H291 is examined in detail for various redox states of the hemes and various conformations of E242 side-chain. Redox potential calculations of the successive steps in the reaction cycle during the O→E transition are able to explain a cascade of equilibria between the different intermediate states and electron redistribution between the metal centers during the course of the catalytic activity. All four electrometric phases are discussed in the light of the obtained results, providing a robust support for the His291 model of proton pumping in CcO.

Spectral components of the α-band of cytochrome oxidase

Oxidative redox titrations of the mitochondrial cytochromes were performed in near-anoxic RAW 264.7 cells by inhibiting complex I. Cytochrome oxidation changes were measured with multi-wavelength spectroscopy and the ambient redox potential was calculated from the oxidation state of endogenous cytochrome c. Two spectral components were separated in the α-band range of cytochrome oxidase and they were identified as the difference spectrum of heme a when it has a high (a(H)) or low (a(L)) midpoint potential (E(m)) by comparing their occupancy during redox titrations carried out when the membrane potential (ΔΨ) was dissipated with a protonophore to that predicted by the neoclassical model of redox cooperativity. The difference spectrum of a(L) has a maximum at 605nm whereas the spectrum of a(H) has a maximum at 602nm. The ΔΨ-dependent shift in the E(m) of a(H) was too great to be accounted for by electron transfer from cytochrome c to heme a against ΔΨ but was consistent with a model in which a(H) is formed after proton uptake against ΔΨ suggesting that the spectral changes are the result of protonation. A stochastic simulation was implemented to model oxidation states, proton uptake and E(m) changes during redox titrations. The redox anti-cooperativity between heme a and heme a(3), and proton binding, could be simulated with a model where the pump proton interacted with heme a and the substrate proton interacted with heme a(3) with anti-cooperativity between proton binding sites, but not with a single proton binding site coupled to both hemes.

Redox Bohr effects and the role of heme a in the proton pump of bovine heart cytochrome c oxidase

Structural and functional observations are reviewed which provide evidence for a central role of redox Bohr effect linked to the low-spin heme a in the proton pump of bovine heart cytochrome c oxidase. Data on the membrane sidedness of Bohr protons linked to anaerobic oxido-reduction of the individual metal centers in the liposome reconstituted oxidase are analysed. Redox Bohr protons coupled to anaerobic oxido-reduction of heme a (and Cu(A)) and Cu(B) exhibit membrane vectoriality, i.e. protons are taken up from the inner space upon reduction of these centers and released in the outer space upon their oxidation. Redox Bohr protons coupled to anaerobic oxido-reduction of heme a(3) do not, on the contrary, exhibit vectorial nature: protons are exchanged only with the outer space. A model of the proton pump of the oxidase, in which redox Bohr protons linked to the low-spin heme a play a central role, is described. This article is part of a Special Issue entitled: Allosteric cooperativity in respiratory proteins.

Multiconformation continuum electrostatics analysis of the effects of a buried Asp introduced near heme a in Rhodobacter sphaeroides cytochrome c oxidase

Cytochrome c oxidase (CcO) reduces O(2) to water via a series of proton-coupled electron transfers, generating a transmembrane electrochemical gradient. Coupling electron and proton transfer requires changing the pK(a) values of buried residues at each stage in the reaction cycle. Heme a is a key cofactor in the CcO electron transfer chain. Mutation of Ser44 to Asp has been reported [Mills, D. A., et al. (2008) Biochemistry 47, 11499-11509], changing the hydrogen bond acceptor from His102, the heme a axial ligand in Rhodobactor sphaeroides CcO. This adds an acidic residue to the CcO interior. The electrochemical behavior of heme a in wild-type and S44D CcO is compared using the continuum electrostatics program MCCE. The introduced, deeply buried Asp remains ionized at physiological pH only when the nearby heme is oxidized. Heme a reduction is now calculated to be strongly coupled to Asp proton binding, while with Ser44, it is weakly coupled to small protonation shifts at multiple sites, increasing the pH dependence in the mutant. At pH 7, the partially ionized Asp 44 is calculated to lower the heme redox potential by 50 mV as expected given the thermodynamics of coupled electron and proton transfers. This highlights an curious finding in the experimental results where a low Asp pK(a) is found together with a stabilized reduced heme. The stabilization of a heme oxidation in a model complex by a hydrogen bond to the axial His ligand calculated with continuum electrostatics and with density functional theory were in good agreement.

Analysis of the electrochemistry of hemes with E(m)s spanning 800 mV

The free energy of heme reduction in different proteins is found to vary over more than 18 kcal/mol. It is a challenge to determine how proteins manage to achieve this enormous range of E(m)s with a single type of redox cofactor. Proteins containing 141 unique hemes of a-, b-, and c-type, with bis-His, His-Met, and aquo-His ligation were calculated using Multi-Conformation Continuum Electrostatics (MCCE). The experimental E(m)s range over 800 mV from -350 mV in cytochrome c(3) to 450 mV in cytochrome c peroxidase (vs. SHE). The quantitative analysis of the factors that modulate heme electrochemistry includes the interactions of the heme with its ligands, the solvent, the protein backbone, and sidechains. MCCE calculated E(m)s are in good agreement with measured values. Using no free parameters the slope of the line comparing calculated and experimental E(m)s is 0.73 (R(2) = 0.90), showing the method accounts for 73% of the observed E(m) range. Adding a +160 mV correction to the His-Met c-type hemes yields a slope of 0.97 (R(2) = 0.93). With the correction 65% of the hemes have an absolute error smaller than 60 mV and 92% are within 120 mV. The overview of heme proteins with known structures and E(m)s shows both the lowest and highest potential hemes are c-type, whereas the b-type hemes are found in the middle E(m) range. In solution, bis-His ligation lowers the E(m) by approximately 205 mV relative to hemes with His-Met ligands. The bis-His, aquo-His, and His-Met ligated b-type hemes all cluster about E(m)s which are approximately 200 mV more positive in protein than in water. In contrast, the low potential bis-His c-type hemes are shifted little from in solution, whereas the high potential His-Met c-type hemes are raised by approximately 300 mV from solution. The analysis shows that no single type of interaction can be identified as the most important in setting heme electrochemistry in proteins. For example, the loss of solvation (reaction field) energy, which raises the E(m), has been suggested to be a major factor in tuning in situ E(m)s. However, the calculated solvation energy vs. experimental E(m) shows a slope of 0.2 and R(2) of 0.5 thus correlates weakly with E(m)s. All other individual interactions show even less correlation with E(m). However the sum of these terms does reproduce the range of observed E(m)s. Therefore, different proteins use different aspects of their structures to modulate the in situ heme electrochemistry. This study also shows that the calculated E(m)s are relatively insensitive to different heme partial charges and to the protein dielectric constant used in the simulation.

The steady-state mechanism of cytochrome c oxidase: redox interactions between metal centres

The steady-state behaviour of isolated mammalian cytochrome c oxidase was examined by increasing the rate of reduction of cytochrome c. Under these conditions the enzyme's 605 (haem a), 655 (haem a3/CuB) and 830 (CuA) nm spectral features behaved as if they were at near equilibrium with cytochrome c (550 nm). This has implications for non-invasive tissue measurements using visible (550, 605 and 655 nm) and near-IR (830 nm) light. The oxidized species represented by the 655 nm band is bleached by the presence of oxygen intermediates P and F (where P is characterized by an absorbance spectrum at 607 nm relative to the oxidized enzyme and F is characterized by an absorbance spectrum at 580 nm relative to the oxidized enzyme) or by reduction of haem a3 or CuB. However, at these ambient oxygen levels (far above the enzyme Km), the populations of reduced haem a3 and the oxygen intermediates were very low (<10%). We therefore interpret 655 nm changes as reduction of the otherwise spectrally invisible CuB centre. We present a model where small anti-cooperative redox interactions occur between haem a–CuA–CuB (steady-state potential ranges: CuA, 212–258 mV; haem a, 254–281 mV; CuB, 227–272 mV). Contrary to static equilibrium measurements, in the catalytic steady state there are no high potential redox centres (>300 mV). We find that the overall reaction is correctly described by the classical model in which the Michaelis intermediate is a ferrocytochrome c–enzyme complex. However, the oxidation of ferrocytochrome c in this complex is not the sole rate-determining step. Turnover is instead dependent upon electron transfer from haem a to haem a3, but the haem a potential closely matches cytochrome c at all times.

A comparison of catalytic site intermediates of cytochrome c oxidase and peroxidases

Compounds I and II of peroxidases such as horseradish peroxidase and cytochrome c peroxidase are relatively well understood catalytic intermediates in terms of their structures and redox states of iron, heme, and associated radical species. The intermediates involved in the oxygen reduction chemistry of the cytochrome c oxidase superfamily are more complicated because of the need for four reducing equivalents and because of the linkage of the oxygen chemistry with vectorial proton translocations. Nevertheless, two of these intermediates, the peroxy and ferryl forms, have characteristics that can in many ways be considered to be counterparts of peroxidase compounds I and II. We explore the primary factors that minimize the generation of unwanted reactive oxygen species products and ensure that the principal enzymological function becomes either that of a peroxidase or an oxidase. These comparisons can provide insights into the nature of biological oxygen reduction chemistry and guidance for the engineering of biomimetic synthetic materials.

Molecular mechanism of proton translocation by cytochrome c oxidase

Cytochrome c oxidase (CcO) is a terminal protein of the respiratory chain in eukaryotes and some bacteria. It catalyzes most of the biologic oxygen consumption on earth done by aerobic organisms. During the catalytic reaction, CcO reduces dioxygen to water and uses the energy released in this process to maintain the electrochemical proton gradient by functioning as a redox-linked proton pump. Even though the structures of several terminal oxidases are known, they are not sufficient in themselves to explain the molecular mechanism of proton pumping. Thus, additional extensive studies of CcO by varieties of biophysical and biochemical approaches are involved to shed light on the mechanism of proton translocation. In this review, we summarize the current level of knowledge about CcO, including the latest model developed to explain the CcO proton-pumping mechanism.

Exploring the proton pump mechanism of cytochrome c oxidase in real time

Cytochrome c oxidase catalyzes most of the biological oxygen consumption on Earth, a process responsible for energy supply in aerobic organisms. This remarkable membrane-bound enzyme also converts free energy from O(2) reduction to an electrochemical proton gradient by functioning as a redox-linked proton pump. Although the structures of several oxidases are known, the molecular mechanism of redox-linked proton translocation has remained elusive. Here, correlated internal electron and proton transfer reactions were tracked in real time by spectroscopic and electrometric techniques after laser-activated electron injection into the oxidized enzyme. The observed kinetics establish the long-sought reaction sequence of the proton pump mechanism and describe some of its thermodynamic properties. The 10-micros electron transfer to heme a raises the pK(a) of a "pump site," which is loaded by a proton from the inside of the membrane in 150 micros. This loading increases the redox potentials of both hemes a and a(3), which allows electron equilibration between them at the same rate. Then, in 0.8 ms, another proton is transferred from the inside to the heme a(3)/Cu(B) center, and the electron is transferred to Cu(B). Finally, in 2.6 ms, the preloaded proton is released from the pump site to the opposite side of the membrane.

Cytochrome c oxidase: chemistry of a molecular machine

The plethora of proposed chemical models attempting to explain the proton pumping reactions catalyzed by the CcO complex, especially the number of recent models, makes it clear that the problem is far from solved. Although we have not discussed all of the models proposed to date, we have described some of the more detailed models in order to illustrate the theoretical concepts introduced at the beginning of this section on proton pumping as well as to illustrate the rich possibilities available for effecting proton pumping. It is clear that proton pumping is effected by conformational changes induced by oxidation/reduction of the various redox centers in the CcO complex. It is for this reason that the CcO complex is called a redox-linked proton pump. The conformational changes of the proton pump cycle are usually envisioned to be some sort of ligand-exchange reaction arising from unstable geometries upon oxidation/reduction of the various redox centers. However, simple geometrical rearrangements, as in the Babcock and Mitchell models are also possible. In any model, however, hydrogen bonds must be broken and reformed due to conformational changes that result from oxidation/reduction of the linkage site during enzyme turnover. Perhaps the most important point emphasized in this discussion, however, is the fact that proton pumping is a directed process and it is electron and proton gating mechanisms that drive the proton pump cycle in the forward direction. Since many of the models discussed above lack effective electron and/or proton gating, it is clear that the major difficulty in developing a viable chemical model is not formulating a cyclic set of protein conformational changes effecting proton pumping (redox linkage) but rather constructing the model with a set of physical constraints so that the proposed cycle proceeds efficiently as postulated. In our discussion of these models, we have not been too concerned about which electron of the catalytic cycle was entering the site of linkage, but merely whether an ET to the binuclear center played a role. However, redox linkage only occurs if ET to the activated binuclear center is coupled to the proton pump. Since all of the models of proton pumping presented here, with the exception of the Rousseau expanded model and the Wikström model, have a maximum stoichiometry of 1 H+/e-, they inadequately explain the 2 H+/e- ratio for the third and fourth electrons of the dioxygen reduction cycle (see Section V.B). One way of interpreting this shortfall of protons is that the remaining protons are pumped by an as yet undefined indirectly coupled mechanism. In this scenario, the site of linkage could be coupled to the pumping of one proton in a direct fashion and one proton in an indirect fashion for a given electron. For a long time, it was assumed that at least some elements of such an indirect mechanism reside in subunit III. While recent evidence argues against the involvement of subunit III in the proton pump, subunit III may still participate in a regulatory and/or structural capacity (Section II.E). Attention has now focused on subunits I and II in the search for residues intimately involved in the proton pump mechanism and/or as part of a proton channel. In particular, the role of some of the highly conserved residues of helix VIII of subunit I are currently being studied by site directed mutagenesis. In our opinion, any model that invokes heme alpha 3 or CuB as the site of linkage must propose a very effective means by which the presumedly fast uncoupling ET to the dioxygen intermediates is prevented. It is difficult to imagine that ET over the short distance from heme alpha 3 or CuB to the dioxygen intermediate requires more than 1 ns. In addition, we expect the conformational changes of the proton pump to require much more than 1 ns (see Section V.B).

Darwin at the molecular scale: selection and variance in electron tunnelling proteins including cytochrome c oxidase

Biological electron transfer is designed to connect catalytic clusters by chains of redox cofactors. A review of the characterized natural redox proteins with a critical eye for molecular scale measurement of variation and selection related to physiological function shows no statistically significant differences in the protein medium lying between cofactors engaged in physiologically beneficial or detrimental electron transfer. Instead, control of electron tunnelling over long distances relies overwhelmingly on less than 14 A spacing between the cofactors in a chain. Near catalytic clusters, shorter distances (commonly less than 7 A) appear to be selected to generate tunnelling frequencies sufficiently high to scale the barriers of multi-electron, bond-forming/-breaking catalysis at physiological rates. We illustrate this behaviour in a tunnelling network analysis of cytochrome c oxidase. In order to surmount the large, thermally activated, adiabatic barriers in the 5-10 kcal mol-1 range expected for H+ motion and O2 reduction at the binuclear centre of oxidase on the 10(3)-10(5) s-1 time-scale of respiration, electron access with a tunnelling frequency of 10(9) or 10(10) s-1 is required. This is provided by selecting closely placed redox centres, such as haem a (6.9 A) or tyrosine (4.9 A). A corollary is that more distantly placed redox centres, such as CuA, cannot rapidly scale the catalytic site barrier, but must send their electrons through more closely placed centres, avoiding direct short circuits that might circumvent proton pumping coupled to haems a to a3 electron transfer. The selection of distances and energetic barriers directs electron transfer from CuA to haem a rather than a3, without any need for delicate engineering of the protein medium to 'hard wire' electron transfer. Indeed, an examination of a large number of oxidoreductases provides no evidence of such naturally selected wiring of electron tunnelling pathways.

Calculated proton uptake on anaerobic reduction of cytochrome C oxidase: is the reaction electroneutral?

Cytochrome c oxidase is a transmembrane proton pump that builds an electrochemical gradient using chemical energy from the reduction of O(2). Ionization states of all residues were calculated with Multi-Conformation Continuum Electrostatics (MCCE) in seven anaerobic oxidase redox states ranging from fully oxidized to fully reduced. One long-standing problem is how proton uptake is coupled to the reduction of the active site binuclear center (BNC). The BNC has two cofactors: heme a(3) and Cu(B). If the protein needs to maintain electroneutrality, then 2 protons will be bound when the BNC is reduced by 2 electrons in the reductive half of the reaction cycle. The effective pK(a)s of ionizable residues around the BNC are evaluated in Rhodobacter sphaeroides cytochrome c oxidase. At pH 7, only a hydroxide coordinated to Cu(B) shifts its pK(a) from below 7 to above 7 and so picks up a proton when heme a(3) and Cu(B) are reduced. Glu I-286, Tyr I-288, His I-334, and a second hydroxide on heme a(3) all have pK(a)s above 7 in all redox states, although they have only 1.6-3.5 DeltapK units energy cost for deprotonation. Thus, at equilibrium, they are protonated and cannot serve as proton acceptors. The propionic acids near the BNC are deprotonated with pK(a)s well below 7. They are well stabilized in their anionic state and do not bind a proton upon BNC reduction. This suggests that electroneutrality in the BNC is not maintained during the anaerobic reduction. Proton uptake on reduction of Cu(A), heme a, heme a(3), and Cu(B) shows approximately 2.5 protons bound per 4 electrons, in agreement with prior experiments. One proton is bound by a hydroxyl group in the BNC and the rest to groups far from the BNC. The electrochemical midpoint potential (E(m)) of heme a is calculated in the fully oxidized protein and with 1 or 2 electrons in the BNC. The E(m) of heme a shifts down when the BNC is reduced, which agrees with prior experiments. If the BNC reduction is electroneutral, then the heme a E(m) is independent of the BNC redox state.

Electron tunneling chains of mitochondria

The single, simple concept that natural selection adjusts distances between redox cofactors goes a long way towards encompassing natural electron transfer protein design. Distances are short or long as required to direct or insulate promiscuously tunneling single electrons. Along a chain, distances are usually 14 A or less. Shorter distances are needed to allow climbing of added energetic barriers at paired-electron catalytic centers in which substrate and the required number of cofactors form a compact cluster. When there is a short-circuit danger, distances between shorting centers are relatively long. Distances much longer than 14 A will support only very slow electron tunneling, but could act as high impedance signals useful in regulation. Tunneling simulations of the respiratory complexes provide clear illustrations of this simple engineering.

Protonmotive cooperativity in cytochrome c oxidase

Cooperative linkage of solute binding at separate binding sites in allosteric proteins is an important functional attribute of soluble and membrane bound hemoproteins. Analysis of proton/electron coupling at the four redox centers, i.e. Cu(A), heme a, heme a(3) and Cu(B), in the purified bovine cytochrome c oxidase in the unliganded, CO-liganded and CN-liganded states is presented. These studies are based on direct measurement of scalar proton translocation associated with oxido-reduction of the metal centers and pH dependence of the midpoint potential of the redox centers. Heme a (and Cu(A)) exhibits a cooperative proton/electron linkage (Bohr effect). Bohr effect seems also to be associated with the oxygen-reduction chemistry at the heme a(3)-Cu(B) binuclear center. Data on electron transfer in cytochrome c oxidase are also presented, which, together with structural data, provide evidence showing the occurrence of direct electron transfer from Cu(A) to the binuclear center in addition to electron transfer via heme a. A survey of structural and functional data showing the essential role of cooperative proton/electron linkage at heme a in the proton pump of cytochrome c oxidase is presented. On the basis of this and related functional and structural information, variants for cooperative mechanisms in the proton pump of the oxidase are examined.

Thermodynamic and choreographic constraints for energy transduction by cytochrome c oxidase

Cooperative effects are fundamental for electroprotonic energy transduction processes, crucial to sustain much of life chemistry. However, the primary cooperative mechanism by which transmembrane proteins couple the downhill transfer of electrons to the uphill activation (acidification) of protic groups is still a matter of great controversy. To understand cooperative processes fully, it is necessary to obtain the microscopic thermodynamic parameters of the functional centres and relate them to the relevant structural features, a task difficult to achieve for large proteins. The approach discussed here explores how this may be done by extrapolation from mechanisms used by simpler proteins operative in similar processes. The detailed study of small, soluble cytochromes performing electroprotonic activation has shown how they use anti-electrostatic effects to control the synchronous movement of charges. These include negative e(-)/H(+) (redox-Bohr effect) cooperativities. This capacity is the basis to discuss an unorthodox mechanism consistent with the available experimental data on the process of electroprotonic energy transduction performed by cytochrome c oxidase (CcO).

Proton transfer reactions associated with the reaction of the fully reduced, purified cytochrome C oxidase with molecular oxygen and ferricyanide

A study is presented on proton transfer associated with the reaction of the fully reduced, purified bovine heart cytochrome c oxidase with molecular oxygen or ferricyanide. The proton consumption associated with aerobic oxidation of the four metal centers changed significantly with pH going from approximately 3.0 H(+)/COX at pH 6.2-6.3 to approximately 1.2 H(+)/COX at pH 8.0-8.5. Rereduction of the metal centers was associated with further proton uptake which increased with pH from approximately 1.0 H(+)/COX at pH 6.2-6.3 to approximately 2.8 H(+)/COX at pH 8.0-8.5. Anaerobic oxidation of the four metal centers by ferricyanide resulted in the net release of 1.3-1.6 H(+)/COX in the pH range 6.2-8.2, which were taken up by the enzyme on rereduction of the metal centers. The proton transfer elicited by ferricyanide represents the net result of deprotonation/protonation reactions linked to anaerobic oxidoreduction of the metal centers. Correction for the ferricyanide-induced pH changes of the proton uptake observed in the oxidation and rereduction phase of the reaction of the reduced oxidase with oxygen gave a measure of the proton consumption in the reduction of O(2) to 2H(2)O. The results show that the expected stoichiometric proton consumption of 4H(+) in the reduction of O(2) to 2H(2)O is differently associated, depending on the actual pH, with the oxidation and reduction phase of COX. Two H(+)/COX are initially taken up in the reduction of O(2) to two OH(-) groups bound to the binuclear Fe a(3)-Cu(B) center. At acidic pHs the third and fourth protons are also taken up in the oxidative phase with formation of 2H(2)O. At alkaline pHs the third and fourth protons are taken up with formation of 2H(2)O only upon rereduction of COX.

A mechano-chemical model for energy transduction in cytochrome c oxidase: the work of a Maxwell's god

Cytochrome c3 has a central role in the energetics of Desulfovibrio sp., where it performs an electroprotonic energy transduction step. This process uses a network of cooperativities, largely based on anti-Coulomb components, resulting from a mechano-chemical energy coupling mechanism. This mechanism provides a model coherent with the data available for the redox chemistry of haem a of cytochrome c oxidase and its link to the activation of protons. A crucial feature of the model is an anti-Coulomb effect that sets the stage for a molecular ratchet, ensuring vectoriality for the redox-driven localised movement of protons across the membrane, against an electrochemical gradient.

pH-dependent structural changes at the Heme-Copper binuclear center of cytochrome c oxidase

The resonance Raman spectra of the aa3 cytochrome c oxidase from Rhodobacter sphaeroides reveal pH-dependent structural changes in the binuclear site at room temperature. The binuclear site, which is the catalytic center of the enzyme, possesses two conformations at neutral pH, assessed from their distinctly different Fe-CO stretching modes in the resonance Raman spectra of the CO complex of the fully reduced enzyme. The two conformations (alpha and beta) interconvert reversibly in the pH 6-9 range with a pKa of 7.4, consistent with Fourier transform infrared spectroscopy measurements done at cryogenic temperatures (D.M. Mitchell, J.P. Sapleigh, A.M.Archer, J.O. Alben, and R.B.Gennis, 1996, Biochemistry 35:9446-9450). It is postulated that the different structures result from a change in the position of the Cu(B) atom with respect to the CO due to the presence of one or more ionizable groups in the vicinity of the binuclear center. The conserved tyrosine residue (Tyr-288 in R. sphaeroides, Tyr-244 in the bovine enzyme) that is adjacent to the oxygen-binding pocket or one of the histidines that coordinate Cu(B) are possible candidates. The existence of an equilibrium between the two conformers at physiological pH and room temperature suggests that the conformers may be functionally involved in enzymatic activity.

Electron transfer rates and equilibrium within cytochrome c oxidase

Intramolecular electron transfer (ET) between the CuA center and heme a in bovine cytochrome c oxidase was investigated by pulse radiolysis. CuA, the initial electron acceptor, was reduced by 1-methyl nicotinamide radicals in a diffusion-controlled reaction, as monitored by absorption changes at 830 nm. After the initial reduction phase, the 830 nm absorption was partially restored, corresponding to reoxidation of the CuA center. Concomitantly, the absorption at 445 nm and 605 nm increased, indicating reduction of heme a. The rate constants for heme a reduction and CuA reoxidation were identical within experimental error and independent of the enzyme concentration. This demonstrates that a fast intramolecular electron equilibration is taking place between CuA and heme a. The rate constants for CuA --> heme a ET and the reverse (heme a --> CuA) process were found to be 13 000 s-1 and 3700 s-1, respectively, at 25 degrees C and pH 7.4. This corresponds to an equilibrium constant of 3.4 under these conditions. Thermodynamic and activation parameters of the ET reactions were determined. The significance of these results, particularly the observed low activation barriers, are discussed within the framework of the known three-dimensional structure, ET pathways and reorganization energies.

Effects of mutation of residue I67 on redox-linked protonation processes in yeast cytochrome c oxidase

We describe effects of a mutation, Ile-67-->Asn, in subunit I of yeast cytochrome c oxidase on redox-linked protonation processes within the protein. The mutation lowers the midpoint potential of haem a and weakens its pH dependency, but has little effect on the potential of haem a3. The residue is close to a conserved glutamate (Glu-243) in the crystal structure. We propose that protonation of Glu-243 is redox-linked to haem a, that Asn-167 perturbs its pK and that redox-linked protonation in this location is essential for the catalytic reactions of the binuclear centre. These proposals are discussed in terms of a 'glutamate trap' mechanism for proton translocation in the haem/copper oxidases.

Cytochrome c oxidase as a proton-pumping peroxidase: reaction cycle and electrogenic mechanism

Cytochrome oxidase (COX) is considered to integrate in a single enzyme two consecutive mechanistically different redox activities--oxidase and peroxidase--that can be catalyzed elsewhere by separate hemoproteins. From the viewpoint of energy transduction, the enzyme is essentially a proton pumping peroxidase with a built-in auxiliary eu-oxidase module that activates oxygen and prepares in situ H2O2, a thermodynamically efficient but potentially hazardous electron acceptor for the proton pumping peroxidase. The eu-oxidase and peroxidase phases of the catalytic cycle may be performed by different structural states of COX. Resolution of the proton pumping peroxidase activity of COX and identification of individual charge translocation steps inherent in this reaction are discussed, as well as the specific role of the two input proton channels in proton translocation.

Protonmotive mechanism of heme-copper oxidases

The mechanism of coupling of proton and electron transfer in oxidases is reviewed and related to the structural information that is now available. A "glutamate trap" mechanism for proton/electron coupling is described.

Structural and functional analysis of deficient mutants in subunit I of cytochrome c oxidase from Saccharomyces cerevisiae

Four point mutations in subunit I of cytochrome c oxidase from Saccharomyces cerevisiae that had been selected for respiratory incompetence but still contained spectrally detectable haem aa3 were analysed. The isolated mutant enzymes exhibited minor band shifts in their optical spectra and contained all eleven subunits. However, steady state activities were only a few percent compared to wild type enzyme. Using a comprehensive experimental approach, we first checked the integrity of the enzyme preparations and then identified the specific functional defect. The results are discussed using information from the recently solved structures of cytochrome c oxidase at 2.8 A. Mutation 167N is positioned between haem a and a conserved glutamate residue (E243). It caused a distortion of the EPR signal of haem a and shifted its midpoint potential by 54 mV to the negative. The high-resolution structure suggests that the primary reason for the low activity of the mutant enzyme could be that asparagine in position 67 might form a stable hydrogen bond to E243, which is part of a proposed proton channel. Cytochrome c oxidase isolated from mutant T316K did not meet our criteria for homogeneity and was therefore omitted from further analysis. Mutants G352V and V380M exhibited an impairment of electron transfer from haem a to a3 and ligand binding to the binuclear centre was affected. In mutant V380M also the midpoint potential of CuB was shifted by 65 mV to the positive. The results indicated for these two mutants changes primarily associated with the binuclear centre, possibly associated with an interference in the routes and/or sites of protonation which are required for stable formation of the catalytic intermediates. This interpretation is discussed in the light of the high resolution structure.

Redox-linked protolytic reactions in soluble cytochrome-c oxidase from beef-heart mitochondria: redox Bohr effects

A study is presented of co-operative redox-linked protolytic reactions (redox Bohr effects) in soluble cytochrome-c oxidase purified from bovine-heart mitochondria. Bohr effects were analyzed by direct measurement, with accurate spectrophotometric and potentiometric methods, of H+ uptake and release by the oxidase associated with reduction and oxidation of hemes a and a3. CuA and CuB in the unliganded and in the CN- or CO-liganded enzyme. The results show that there are in the bovine oxidase four protolytic groups undergoing reversible pK shifts upon oxido-reduction of the electron transfer metals. Two groups with pKox and pKred values around 7 and > 12 respectively appear to be linked to redox transitions of heme a3. One group with pKox and pKred around 6 and 7 is apparently linked to CuB, a fourth one with pKox and pKred of 6 and 9 appears to be linked to heme a. The possible nature of the amino acids involved in the redox Bohr effects and their role in H+ translocation is discussed.

Carboxyl group protonation upon reduction of the Paracoccus denitrificans cytochrome c oxidase: direct evidence by FTIR spectroscopy

The redox reactions of the cytochrome c oxidase from Paracoccus denitrificans were investigated in a thin-layer cell designed for the combination of electrochemistry under anaerobic conditions with UV/VIS and IR spectroscopy. Quantitative and reversible electrochemical reactions were obtained at a surface-modified electrode for all cofactors as indicated by the optical signals in the 400-700 nm range. Fourier transform infrared (FTIR) difference spectra of reduction and oxidation (reduced-minus-oxidized and oxidized-minus-reduced, respectively) obtained in the 1800-1000 cm(-1) range reveal highly structured band features with major contributions in the amide I (1620-1680 cm(-1)) and amide II (1580-1520 cm(-1)) range which indicate structural rearrangements in the cofactor vicinity. However, the small amplitude of the IR difference signals indicates that these conformational changes are small and affect only individual peptide groups. In the spectral region above 1700 cm(-1), a positive peak in the reduced state (1733 cm(-1)) and negative peak in the oxidized st ate (1745 cm(-1)) are characteristic for the formation and decay of a COOH mode upon reduction. The most obvious interpretation of this difference signal is proton uptake by one Asp or Glu side chain carboxyl group in the reduced state and deprotonation of another Asp or Glu residue. Moreover, both residues could well be coupled as a donor-acceptor pair in the proton transfer chain. An alternative interpretation is in terms of a protonated carboxyl group which shifts to a different environment in the reduced state. The relevance of this first direct observation of protein protonation changes in the cytochrome c oxidase for vectorial proton transfer and the catalytic reaction is discussed.

Interconversion of fast and slow forms of cytochrome bo from Escherichia coli

The fully oxidized fast form of cytochrome bo from Escherichia coli is shown to convert spontaneously to a slow form when stored at -20 degrees C in 50 mM potassium borate, pH 8.5, containing 0.5 mM potassium EDTA. Evidence for the conversion, and that the form produced is analogous to the slow form of bovine heart cytochrome c oxidase, comes from (a) decreases in the extents of fast (k = 1-2 x 10(3) M-1 s-1) H2O2 binding and fast (k = 20-30 M-1 s-1) cyanide binding; (b) changes in the optical spectrum that are like those induced by formate, i.e., a blue shift in the Soret absorption band, loss of absorbance in the alpha and beta bands, and a red shift in the "630 nm" charge-transfer band; (c) changes in the EPR spectrum that are like those induced by formate, i.e., disappearance of signals at g = 8.6 and g = 3.71, and appearance of signals at g approximately 13, g = 3.14, and g = 2.58; and (d) appearance of a slow phase of reduction of heme o by dithionite. The mutant enzyme E286Q also converts to a slow form under the same conditions, as shown by (a) a decrease in the extent of fast H2O2 binding; (b) changes in the optical spectrum like those seen with wild-type enzyme; and (c) changes in the EPR spectrum that are like those induced by formate, i.e., disappearance of signals at g = 7.3 and g = 3.6 and appearance of signals at g approximately 13, g = 3.18, and g = 2.59.(ABSTRACT TRUNCATED AT 250 WORDS)

Rapid electron injection into multisite metalloproteins: intramolecular electron transfer in cytochrome oxidase

The principles for the operation of redox-linked proton pumps are reviewed and applied to one specific pump, cytochrome oxidase. Systematic studies of internal electron transfer in the different redox states of this pump will be facilitated by the development of methods for rapid electron injection into the metal centers of the enzyme. Two methods that have been employed to generate electron donors are pulse radiolysis and laser flash photolysis. The rate of electron injection from photoexcited Ru-modified cytochrome c or triplet Zn-cytochrome c into the CuA center is about 10(5) s-1, and the CuA/cytochrome a electron equilibration rate is 2 x 10(4) s-1. Electron transfer from cytochrome a to the cytochrome a3-CuB site occurs at 2 x 10(5) s-1 in the half-reduced enzyme, whereas the rate is only 2 x 10(2) s-1 in the peroxide intermediate, despite a much higher driving force. It is likely that variations in distant electronic coupling attributable to a ligand shuttle, as well as changes in the reorganization energy of one or more of the redox centers, contribute to the control of internal electron flow in the enzyme.

Mechanistic and phenomenological features of proton pumps in the respiratory chain of mitochondria

Various direct, indirect (kinetic and thermodynamic), and combined mechanisms have been proposed to explain the conversion of redox energy into a transmembrane protonmotive force (delta p) by enzymatic complexes of respiratory chains. The conceptual evolution of these models is examined. The characteristics of thermodynamic coupling between redox transitions of electron carriers and scalar proton transfer in cytochrome c oxidase and its possible involvement in proton pumping is discussed. Other aspects dealt with in this paper are: (i) variability of <--H+/e- stoichiometries, in cytochrome c oxidase and cytochrome c reductase and its mechanistic implications; (ii) possible models by which the reduction of dioxygen to water at the binuclear heme-copper center of protonmotive oxidases can be directly involved in proton pumping. Finally a unifying concept for proton pumping by the redox complexes of respiratory chain is presented.

Proton uptake by cytochrome c oxidase on reduction and on ligand binding

On reduction, cytochrome oxidase was found to take up 2.4 +/- 0.1 protons in the pH range 7.2-8.5, of which 2 are associated with the binuclear centre, and the remaining fractional proton with haem a/CuA. Ligation to oxidised cytochrome oxidase of the azide, formate, fluoride or cyanide anions is accompanied by uptake of one proton. In the case of the reduced enzyme, no protonation changes are observed on binding O2 (Hallén S. and Nilsson T. (1992) Biochemistry 31, 11853-11859) or CO. Cyanide binding to reduced oxidase is, in contrast, still accompanied by uptake of a proton. These findings are discussed in terms of our previously-published proposal for the ligand chemistry of the binuclear site. The results overall suggest a principle of electroneutrality of redox and ligand state changes of the binuclear centre, with charge compensations provided only by protonation reactions.

Stoichiometry and redox behaviour of metals in cytochrome-c oxidase

The early observation of extra copper in preparations of cytochrome-c oxidase has recently lead to a renewed interest in its stoichiometry and possible redox function. In various, pure preparations (heme A contents close to the theoretical value of 9.79 nmol/mg protein for the 13-subunit bovine enzyme) protein-related metal stoichiometries of 3 Cu, 2 Fe, 1 Zn, 1 Mg/monomer with M(r) 204266 were determined. Despite the presence of five potential redox metal ions, reductive and reoxidative titrations indicate the presence of only four one-electron-accepting/donating species in the ligand-free enzyme. Participation of two copper ions in a binuclear copper site acting as one-electron acceptor may explain both the observed copper stoichiometry and the redox behaviour. The homology of the C-terminal sequence of subunit II with one of the copper-binding sites in nitrous-oxide reductases provides possible ligands for complexing two copper ions in a binuclear center.

Proton translocation in cytochrome c oxidase: redox linkage through proximal ligand exchange on cytochrome a3

An analysis of resonance Raman scattering data from CO-bound cytochrome c oxidase and from the photodissociated enzyme indicates that histidine may not be coordinated to the iron atom of cytochrome a3 in the CO-bound form of the enzyme. Instead, the data suggest that either a water molecule or a different amino acid residue occupies the proximal ligand position. From these data, it is postulated that ligand exchange on cytochrome a3 can occur under physiological conditions. Studies of mutant hemoglobins have demonstrated that tyrosinate binds preferentially to histidine in the ferric forms of the proteins. In cytochrome c oxidase tyrosine residues are located near the histidine residues recently implicated in coordination to cytochrome a3 (Shapleigh et al., 1992; Hosler et al., this volume). Expanding on these concepts, we propose a model for proton translocation at the O2-binding site based on proximal ligand exchange between tyrosine and histidine on cytochrome a3. The pumping steps take place at the level of the peroxy intermediate and at the level of the ferryl intermediate in the catalytic cycle and are thereby consistent with the recent results of Wilkstrom (1989) who found that proton pumping occurs only at these two steps. It is shown that the model may be readily extended to account for the pumping of two protons at each of the steps.

Non-linear inhibition curves for tight-binding inhibitors of dimeric ubiquinol-cytochrome c oxidoreductases. Evidence for rapid inhibitor mobility

Steady-state electron flow through and electron delivery into isolated dimeric bc1 complex (ubiquinol--cytochrome c oxidoreductase) from Neurospora crassa and beef heart mitochondria were studied in the presence of increasing concentrations of antimycin A, funiculosin and/or myxothiazol. Parabolic or linear inhibition curves were obtained, depending upon the different quinols and inhibitors that were used. Linear curves occur when the inhibitor directly affects the rate-determining step. The most reasonable explanation for the parabolic curves is given by a fast intradimeric exchange of the hydrophobic inhibitors antimycin A, funiculosin (rate less than 500 s-1) and of myxothiazol (rate greater than 1 s-1). Using mitochondria from beef heart, the shape of the inhibition curve with antimycin A is parabolic if the quinol--O2 oxidoreductase turns over at about 300 s-1, but hyperbolic if the rate is 5 times less. The hyperbolic titration curve may be the result of both intradimeric and an additional interdimeric redistribution (rate approximately 100 s-1) of inhibitors between enzymes incorporated in a continuous phospholipid membrane. This explanation is supported by experiments with chromatophores obtained from Rhodobacter capsulatus. As recently described [Fernandez-Velasco, J. & Crofts, A. R. (1992) Biophys. J. 2, A153], cytochrome b becomes fully reoxidized within 1 s after a flash at substoichiometric concentrations of antimycin A. This kinetic of the slow reoxidation can be expressed in terms of the intradimeric and interdimeric redistribution with rate constants of about 10 s-1 and 2 x 10(6) M-1 s-1, respectively. It seems that rapid inhibitor redistribution may be a widespread phenomenon for hydrophobic inhibitors of enzymes incorporated in lipid membranes.

Photoinduced electron transfer from tris(2,2'-bipyridyl)ruthenium to cytochrome c oxidase

Flash photolysis has been used to effect electron transfer from tris(2,2'-bipyridyl)ruthenium(II) to cytochrome c oxidase in the presence of a sacrificial electron donor, aniline. The observation that photoreduction occurs only at low ionic strength and high pH indicates that an electrostatic complex between the ruthenium compound and the enzyme is the reactive species. The reaction was followed at 830, 605, and 445 nm. The initial absorbance changes observed suggest that the copper ion CuA is the preferred electron acceptor and that electron transfer from the excited ruthenium complex takes place in less than 1 microsecond. Some rapid cytochrome a reduction is also observed. Absorbance changes after the initial transients suggest that the reduced CuA then equilibrates with cytochrome a with a rate constant of 2 x 10(4) s-1. Comparison of the absorbance changes at 605 and 445 nm and the kinetic difference spectrum in the Soret region indicate that no reduction of cytochrome a3 takes place. With the oxidized enzyme, no further reactions were detected, whereas, in the peroxide and ferryl intermediates, cytochrome a reoxidizes on a millisecond time scale. The reaction appears biphasic in both intermediates, with rate constants in the range 2 x 10(2) to 4 x 10(3) s-1. This is considerably slower than the maximal rates observed for electron transfer between cytochrome a and the bimetallic site found in earlier work and suggests rate limitation by other processes. The rates obtained for the slower phases are close to the rate for catalysis of cytochrome c oxidation.