Coupling in cytochrome c oxidase

Cytochrome c oxidase (ferrocytochrome c: oxygen oxidoreductase; EC 1.9.3.1) can be resolved into an electron transfer complex (ETC) and an ionophore transfer complex (ITC). Coupling requires an interaction between the moving electron in the ETC and a moving, positively charged ionophore-cation adduct in the ITC. The duplex character of cytochrome oxidase facilitates this interaction. The ITC mediates cyclical cation transport. It can be replaced as the coupling partner by the combination of valinomycin and nigericin in the presence of K(+) when cytochrome oxidase is incorporated into liposomes containing acidic phospholipids or by the combination of lipid cytochrome c and bile acids in an ITC-resolved preparation of the ETC. Respiratory control can be induced by incorporating cytochrome oxidase into vesicles of unfractionated whole mitochondrial lipid. The activity of the ITC is suppressed by such incorporation and this suppression leads to the emergence of respiratory control. The ionophoroproteins of the ITC can be extracted into organic solvents; some 50% of the total protein of cytochrome oxidase is extractable. The release of free ionophore is achieved by tryptic digestion of the ionophoroprotein. Preliminary to this release the ionophoroprotein is degraded to an ionophoropeptide. Electrogenic ionophores, as well as uncoupler, are liberated by such proteolysis. The ITC contains a set of ionophoroproteins imbedded in a matrix of phospholipid.     

Interheme electron tunneling in cytochrome c oxidase

Cytochrome c oxidase (CcO) is the terminal enzyme of the respiratory chain that catalyzes respiratory reduction of dioxygen (O(2)) to water in all eukaryotes and many aerobic bacteria. CcO, and its homologs among the heme-copper oxidases, has an active site composed of an oxygen-binding heme and a copper center in the vicinity, plus another heme group that donates electrons to this site. In most oxidoreduction enzymes, electron transfer (eT) takes place by quantum-mechanical electron tunneling. Here we show by independent molecular dynamics and quantum-chemical methods that the heme-heme eT in CcO differs from the majority of cases in having an exceptionally low reorganization energy. We show that the rate of interheme eT in CcO may nevertheless be predicted by the Moser-Dutton equation if reinterpreted as the average of the eT rates between all individual atoms of the donor and acceptor weighed by the respective packing densities between them. We argue that this modification may be necessary at short donor/acceptor distances comparable to the donor/acceptor radii.     

Rapid electrostatic evolution at the binding site for cytochrome c on cytochrome c oxidase in anthropoid primates

Cytochrome c (CYC) oxidase (COX), a multisubunit enzyme that functions in mitochondrial aerobic energy production, catalyzes the transfer of electrons from CYC to oxygen and participates in creating the electrochemical gradient used for ATP synthesis. Modeling three-dimensional structural data on COX and CYC reveals that 57 of the >1,500 COX residues can be implicated in binding CYC. Because of the functional importance of the transfer of electrons to oxygen, it might be expected that natural selection would drastically constrain amino acid replacement rates of CYC and COX. Instead, in anthropoid primates, although not in other mammals, CYC and COX show markedly accelerated amino acid replacement rates, with the COX acceleration being much greater at the positions that bind CYC than at those that do not. Specifically, in the anthropoid lineage descending from the last common ancestor of haplorhines (tarsiers and anthropoids) to that of anthropoids (New World monkeys and catarrhines) and that of catarrhines (Old World monkeys and apes, including humans), a minimum of 27 of the 57 COX amino acid residues that bind CYC were replaced, most frequently from electrostatically charged to noncharged residues. Of the COX charge-bearing residues involved in binding CYC, half (11 of 22) have been replaced with uncharged residues. CYC residues that interact with COX residues also frequently changed, but only two of the CYC changes altered charge. We suggest that reducing the electrostatic interaction between COX and CYC was part of the adaptive evolution underlying the emergence of anthropoid primates.     

Properties of a copper-containing cytochrome c1aa3 complex: a terminal oxidase of the extreme thermophile Thermus thermophilus HB8.

From the plasma membrane of Thermus thermophilus HB8 we have partially purified a detergent-solubilized complex of cytochromes a and c1 that actively catalyzes the transfer of electrons from ascorbate via a redox dye to oxygen. The complex is composed of two types of polypeptides, with molecular weights of approximately 55,000 and 33,000. Quantitative analysis revealed the presence of heme a, heme c, and copper in a ratio of 2:1:2, with the heme a being present at 10 +/- 1.3 nmol/mg of protein. The heme c was shown to be associated with the molecular weight 33,000 peptide and is suggested to be of the c1 type. The optical and electron paramagnetic resonance properties of this complex were found to be similar to those of eukaryotic cytochrome oxidase, suggesting the following arrangement of chromophores: a magnetically isolated cytochrome c1 and an oxygen-reducing functional unit consisting of two heme a groups and two copper ions associated with one or more larger peptides.     

CO impedes superfast O2 binding in ba3 cytochrome oxidase from Thermus thermophilus

Kinetic studies of heme-copper terminal oxidases using the CO flow-flash method are potentially compromised by the fate of the photodissociated CO. In this time-resolved optical absorption study, we compared the kinetics of dioxygen reduction by ba(3) cytochrome c oxidase from Thermus thermophilus in the absence and presence of CO using a photolabile O(2)-carrier. A novel double-laser excitation is introduced in which dioxygen is generated by photolyzing the O(2)-carrier with a 355 nm laser pulse and the fully reduced CO-bound ba(3) simultaneously with a second 532-nm laser pulse. A kinetic analysis reveals a sequential mechanism in which O(2) binding to heme a(3) at 90 μM O(2) occurs with lifetimes of 9.3 and 110 μs in the absence and presence of CO, respectively, followed by a faster cleavage of the dioxygen bond (4.8 μs), which generates the P intermediate with the concomitant oxidation of heme b. The second-order rate constant of 1 × 10(9) M(-1) s(-1) for O(2) binding to ba(3) in the absence of CO is 10 times greater than observed in the presence of CO as well as for the bovine heart enzyme. The O(2) bond cleavage in ba(3) of 4.8 μs is also approximately 10 times faster than in the bovine enzyme. These results suggest important structural differences between the accessibility of O(2) to the active site in ba(3) and the bovine enzyme, and they demonstrate that the photodissociated CO impedes access of dioxygen to the heme a(3) site in ba(3), making the CO flow-flash method inapplicable.     

Heme transfer to the heme chaperone CcmE during cytochrome c maturation requires the CcmC protein, which may function independently of the ABC-transporter CcmAB

Cytochrome c maturation in Escherichia coli requires the ccm operon, which encodes eight membrane proteins (CcmABCDEFGH). CcmE is a periplasmic heme chaperone that binds heme covalently and transfers it onto apocytochrome c in the presence of CcmF, CcmG, and CcmH. In this work we addressed the functions of the ccmABCD gene products with respect to holo-CcmE formation and the subsequent ligation of heme to apocytochrome c. In the absence of the ccmABCD genes, heme is not bound to CcmE. We report that CcmC is functionally uncoupled from the ABC transporter subunits CcmA and CcmB, because it is the only Ccm protein that is strictly required for heme transfer and attachment to CcmE. Site-directed mutagenesis of conserved histidines inactivates the CcmC protein, which is in agreement with the hypothesis that this protein interacts directly with heme. We also present evidence that questions the role of CcmAB as a heme exporter; yet, the transported substrate remains unknown. CcmD was found to be involved in stabilizing the heme chaperone CcmE in the membrane. We propose a heme-trafficking pathway as part of a substantially revised model for cytochrome c maturation in E. coli.     

Redox conformation changes in refined tuna cytochrome c.

Tuna ferrocytochrome c and ferricytochrome c have been refined independently at high resolution (1.5 A and 1.8 A) to crystallographic residual errors of 17.3% and 20.8%, respectively. Small but significant conformational differences are seen surrounding a buried water molecule that is hydrogen bonded to Asn-52, Tyr-67, and Thr-78. In the oxidized state, this water molecule is 1.0 A closer to the heme and the heme has moved 0.15 A out of its heme crevice; both changes lead to a more polar microenvironment for the heme. Chemical modification studies, patterns of evolutionary conservatism, structural differences in bacterial cytochromes, and x-ray studies all agree that the "active site" for cytochrome c is bounded by lysines 8, 13,27, 72, 79, 86, and 87 (thus containing the evolutionary conservative 72-87 loop) and has the buried water molecule just below its surface and the opening of the heme crevice slightly to one side.     

Possible proton relay pathways in cytochrome c oxidase.

As the final electron acceptor in the respiratory chain of eukaryotic and many prokaryotic organisms, cytochrome c oxidase (EC 1.9.3.1) catalyzes the reduction of oxygen to water and generates a proton gradient. To test for proton pathways through the oxidase, site-directed mutagenesis was applied to subunit I of the Rhodobacter sphaeroides enzyme. Mutants were characterized in three highly conserved regions of the peptide, comprising possible proton loading, unloading, and transfer sites: an interior loop between helices II and III (Asp132Asn/Ala), an exterior loop between helices IX and X (His411Ala, Asp412Asn, Thr413Asn, Tyr414Phe), and the predicted transmembrane helix VIII (Thr352Ala, Pro358Ala, Thr359Ala, Lys362Met). Most of the mutants had lower activity than wild type, but only mutants at residue 132 lost proton pumping while retaining electron transfer activity. Although electron transfer was substantially inhibited, no major structural alteration appears to have occurred in D132 mutants, since resonance Raman and visible absorbance spectra were normal. However, lower CO binding (70-85% of wild type) suggests some minor change to the binuclear center. In addition, the activity of the reconstituted Asp132 mutants was inhibited rather than stimulated by ionophores or uncoupler. The inhibition was not observed with the purified enzyme and a direct pH effect was ruled out, suggesting an altered response to the electrical or pH gradient. The results support an important role for the conserved II-III loop in the proton pumping process and are consistent with the possibility of involvement of residues in helix VIII and the IX-X loop.     

On the redox conformational change in cytochrome c.

The relationship between the crystal structures of oxidized and reduced tuna cytochrome c has been reexamined by a superposition method motivated by recent studies of the cytochrome c-cytochrome c peroxidase complex. It is shown that the observed structural changes precisely reflect the binding face suggested by chemical modification studies. It is further suggested that the large observed motion of lysine-27 and a smaller overall motion of the two binding edges constitute a redox binding-affinity switch and that the driving force for the conformational change of the protein is provided by the internal conformational change and charge redistribution of the heme, which cause it to tilt, under the influence of covalent and nonbonded interactions, within its protein envelope. A picture is presented of the molecule as an electron storage/transfer machine with three elements--a binding module, an electron storage module, and a conformational energy-storage module.     

Electron transfer between hemes in mammalian cytochrome c oxidase

Fast intraprotein electron transfer reactions associated with enzymatic catalysis are often difficult to synchronize and therefore to monitor directly in non-light-driven systems. However, in the mitochondrial respiratory enzyme cytochrome oxidase aa(3), the kinetics of the final electron transfer step into the active site can be determined: reverse electron flow between the close-lying and chemically identical hemes a(3) and a can be initiated by flash photolysis of CO from reduced heme a(3) under conditions where heme a is initially oxidized. To follow this reaction, we used transient absorption spectroscopy, with femtosecond time resolution and a time window extending to 4 ns. Comparison of the picosecond heme a(3)-CO photodissociation spectra under different redox states of heme a shows significant spectral interaction between both hemes, a phenomenon complicating the interpretation of spectral studies with low time resolution. Most importantly, we show that the intrinsic electron equilibration, corresponding to a DeltaG(0) of 45-55 meV, occurs in 1.2 +/- 0.1 ns. This is 3 orders of magnitude faster than the previously established equilibration phase of approximately 3 mus, which we suggest to reflect a change in redox equilibrium closely following CO migration out of the active site. Our results allow testing a number of conflicting predictions regarding this reaction between both experimental and theoretical studies. We discuss the potential physiological relevance of fast equilibration associated with this low-driving-force redox reaction.     

Axial interactions in the mixed-valent CuA active site and role of the axial methionine in electron transfer

Within Cu-containing electron transfer active sites, the role of the axial ligand in type 1 sites is well defined, yet its role in the binuclear mixed-valent Cu_A sites is less clear. Recently, the mutation of the axial Met to Leu in a Cu_A site engineered into azurin (Cu_A Az) was found to have a limited effect on E⁰ relative to this mutation in blue copper (BC). Detailed low-temperature absorption and magnetic circular dichroism, resonance Raman, and electron paramagnetic resonance studies on Cu_A Az (WT) and its M123X (X = Q, L, H) axial ligand variants indicated stronger axial ligation in M123L/H. Spectroscopically validated density functional theory calculations show that the smaller ΔE⁰ is attributed to H₂O coordination to the Cu center in the M123L mutant in Cu_A but not in the equivalent BC variant. The comparable stabilization energy of the oxidized over the reduced state in Cu_A and BC (Cu_A ∼ 180 mV; BC ∼ 250 mV) indicates that the S(Met) influences E⁰ similarly in both. Electron delocalization over two Cu centers in Cu_A was found to minimize the Jahn–Teller distortion induced by the axial Met ligand and lower the inner-sphere reorganization energy. The Cu–S(Met) bond in oxidized Cu_A is weak (5.2 kcal/mol) but energetically similar to that of BC, which demonstrates that the protein matrix also serves an entatic role in keeping the Met bound to the active site to tune down E⁰ while maintaining a low reorganization energy required for rapid electron transfer under physiological conditions.Long-range electron transfer (ET) is vital to a wide range of biological processes, including two key energy transduction pathways essential for life: H₂O oxidation in photosynthesis and O₂ reduction in respiration (1, 2). Nature has adapted a conserved cupredoxin fold motif (i.e., the Greek-key β barrel) to construct two evolutionarily linked, but structurally distinct Cu-containing ET proteins (3–5). These are the mononuclear type 1 (T1) or blue copper (BC) and binuclear purple Cu_A proteins. The first coordination sphere of the classic BC sites [e.g., plastocyanin (Pc) and azurin (Az)] consists of a trigonally distorted tetrahedral environment where Cu resides in an equatorial plane formed by one S(Cys) and two N(His) ligands and has an axial S(Met) ligand (Fig. 1A) (6, 7). The binuclear purple Cu_A site consists of two bridging S(Cys) ligands and two equatorial N(His) ligands as well as an axial polypeptide backbone carbonyl oxygen [O(Gln) on Cu_O] and an axial thioether sulfur [S(Met) on Cu_M] (Fig. 1B) (8–11). Both sites carry out rapid, efficient long-range ET with rates on the order of 10³–10⁵ s⁻¹ (12, 13).Open in a separate windowFig. 1.The active sites of two previously published Cu ET proteins: (A) the monomeric T1 Cu Az from Pseudomonas aeruginosa (PDB ID code 4AZU) and (B) the binuclear purple Cu_A from T. thermophilus (PDB ID code 2CUA).Although BC proteins use a Cu⁺/Cu²⁺ redox couple, the binuclear Cu_A sites use a (Cu¹⁺–Cu¹⁺)/(Cu^1.5+–Cu^1.5+) redox cycle. The oxidized form of Cu_A is mixed-valent (MV), with a highly covalent Cu₂S₂ core that gives rise to its unique spectroscopic features. The unpaired electron is fully delocalized over the two Cu centers and exhibits a characteristic seven-line ^63,65Cu hyperfine splitting pattern in electron paramagnetic resonance (EPR) spectroscopy (14, 15). Maintaining valence delocalization even in the presence of a low symmetry protein environment has been attributed to the large electronic coupling (H_AB) resulting from a direct Cu–Cu σ bond and efficient superexchange facilitated by substantial Cu₂–S(Cys)₂ covalency. This strong electronic coupling between the two Cu’s leads to a Ψ → Ψ* (Cu–Cu σ → σ*) transition at ∼13,500 cm⁻¹ (16). Excitation into this transition using resonance Raman (RR) yields a large excited state distortion in the totally symmetric Cu₂S₂ core “accordion” mode (ν₁), a characteristic of Robin & Day class III MV delocalization (17–19). The two bridging S(Cys) ligands give rise to four in-plane S(p)-derived molecular orbitals (MOs) for S(Cys) → Ψ* charge transfer (CT) transitions. These have been assigned to absorption bands in the region of 20,000 cm⁻¹. Laser excitation into these CT transitions gives rise to RR enhancement of three additional Cu₂S₂ core vibrations (SI Appendix, Fig. S1A). The functional advantage of a valence delocalization in terms of rapid, long-range ET at low driving forces (∼45 mV) has been ascribed to lowering the reorganization energy (λ) by distributing structural rearrangements associated with redox over two Cu centers (20).In nature, the S(Met) ligand of BC is sometimes found to be replaced by other protein residues. These can either coordinate to Cu [e.g., O(Gln) in stellacyanin (St)] or leave the axial position vacant (e.g., Leu in the fungal laccases) (21, 22). In BC, it was found that variation of the axial ligand from O(Gln) to S(Met) to nothing can tune E⁰ over a 300 mV range (23). In nitrite reductase (NiR), the Cu²⁺–S(Met) bond strength could be experimentally determined and was found to be weak (4.6 kcal/mol) as its loss is compensated by an increased S(Cys) donor interaction with Cu. The low strength of this bond suggested an important role of the protein in keeping the S(Met) ligand bound at physiological temperature. The contribution of the protein in stabilizing the active site structure has been referred to as an entatic/rack state in bioinorganic chemistry (24, 25). For BC sites, the protein matrix provides the negative free energy required to overcome the entropically favored S(Met) bond loss. This plays an important role in ET function as S(Met) binding stabilizes the oxidized more than the reduced state of the Cu site and lowers E⁰ by ∼200 mV.In contrast to BC proteins, S(Met) is the only axial ligand found in naturally occurring Cu_A sites [cytochrome c oxidase (CcO), nitrous oxide reductase (N₂OR), nitric oxide reductase (NOR), terminal oxidase in Sulfolobus acidocaldarius (SoxH)] (26). Interestingly, in contrast to BC, the Met to Leu mutation in the Cu_A Az only led to a 16 mV increase in E⁰ (compared with an 86 mV increase for this mutant in BC Az) (27). This apparent difference in the extent of the axial ligand contribution to E⁰ relative to previous studies on BC has led us to further explore its contribution to function in Cu_A and whether or not it is entatic as in BC. We use a combination of spectroscopic methods [low-temperature (LT) absorption and magnetic circular dichroism (MCD), RR, and EPR] coupled to density functional theory (DFT) calculations to investigate the geometric and electronic structures of Cu_A Az and a series of its axial ligand variants (M123X; X = Q, L, H). The influence of the axial ligand on the E⁰ and λ are evaluated and compared with these properties in the well-understood BC site. Furthermore, the proposed involvement of Cu_A in ET pathways (28) as well as the entatic/rack nature of the Cu–S(Met) bond in Cu_A are evaluated and discussed.     

The timing of proton migration in membrane-reconstituted cytochrome c oxidase

In mitochondria and aerobic bacteria energy conservation involves electron transfer through a number of membrane-bound protein complexes to O2. The reduction of O2, accompanied by the uptake of substrate protons to form H2O, is catalyzed by cytochrome c oxidase (CcO). This reaction is coupled to proton translocation (pumping) across the membrane such that each electron transfer to the catalytic site is linked to the uptake of two protons from one side and the release of one proton to the other side of the membrane. To address the mechanism of vectorial proton translocation, in this study we have investigated the solvent deuterium isotope effect of proton-transfer rates in CcO oriented in small unilamellar vesicles. Although in H2O the uptake and release reactions occur with the same rates, in D2O the substrate and pumped protons are taken up first (tau(D) congruent with 200 micros, "peroxy" to "ferryl" transition) followed by a significantly slower proton release to the other side of the membrane (tau(D) congruent with 1 ms). Thus, the results define the order and timing of the proton transfers during a pumping cycle. Furthermore, the results indicate that during CcO turnover internal electron transfer to the catalytic site is controlled by the release of the pumped proton, which suggests a mechanism by which CcO orchestrates a tight coupling between electron transfer and proton translocation.     

Increase in apparent compressibility of cytochrome c upon oxidation.

The apparent molal adiabatic compressibilities of ferri- and ferrocytochrome c have been determined from measurements of density and sound velocity. The values found were +2.99 X 10(-8) and -2.40 X 10(-8) cm5 mol-1 dyne-1 for the ferri and ferro forms, respectively. Experiments were performed on identical solutions containing either the oxidized or reduced form of protein. Solutions of ferricytochrome c were found to have significantly greater adiabatic compressibility than equivalent solutions of ferrocytochrome c at 25 degrees C and pH 7.15. The remarkable similarity of the three-dimensional structures of the ferri and ferro proteins [Takano, T. & Dickerson, R.E. (1980) Proc. Natl. Acad. Sci. USA 77, 6371-6375] strongly suggests that this difference in compressibility is due to an increase in volume fluctuations within ferricytochrome c relative to the ferro form rather than a change in equilibrium structure or hydration. Such a difference in the dynamic properties of the structures is consistent with both the crystallographic thermal B factors and the observed increase in amide hydrogen exchange kinetics when ferrocytochrome c is oxidized. The relative magnitude of the root mean square volume fluctuations is approximated from an ideal solution treatment of the compressibility data and yields a ratio of delta Vrms (ferri cyt c)/ delta Vrms (ferro cyt c) = 1.3.     

Kinetic gating of the proton pump in cytochrome c oxidase

Cytochrome c oxidase (CcO), the terminal enzyme of the respiratory chain, reduces oxygen to water and uses the released energy to pump protons across a membrane. Here, we use kinetic master equations to explore the energetic and kinetic control of proton pumping in CcO. We construct models consistent with thermodynamic principles, the structure of CcO, experimentally known proton affinities, and equilibrium constants of intermediate reactions. The resulting models are found to capture key properties of CcO, including the midpoint redox potentials of the metal centers and the electron transfer rates. We find that coarse-grained models with two proton sites and one electron site can pump one proton per electron against membrane potentials exceeding 100 mV. The high pumping efficiency of these models requires strong electrostatic couplings between the proton loading (pump) site and the electron site (heme a), and kinetic gating of the internal proton transfer. Gating is achieved by enhancing the rate of proton transfer from the conserved Glu-242 to the pump site on reduction of heme a, consistent with the predictions of the water-gated model of proton pumping. The model also accounts for the phenotype of D-channel mutations associated with loss of pumping but retained turnover. The fundamental mechanism identified here for the efficient conversion of chemical energy into an electrochemical potential should prove relevant also for other molecular machines and novel fuel-cell designs.     

Functional expression of rat cytochrome c in Saccharomyces cerevisiae.

To determine whether a mammalian cytochrome c could efficiently replace iso-1-cytochrome c, which is encoded by the yeast CYC1 gene, the coding sequence of RC9 (a nondefective processed gene from rat) was cloned in both single- and multiple-copy expression vectors under the direction of the yeast alcohol dehydrogenase 1 (ADC1) promoter. Upon transformation of a CYC1 deletion strain, the multiple-copy construct restored a wild-type growth rate on lactate medium; such growth normally requires derepressed amounts of iso-1-cytochrome c. These transformants expressed a level of hybrid ADC1/RC9 mRNA approximately 5- to 10-fold greater than the amount of message from the endogenous ADC1 gene and produced a steady-state level of rat cytochrome c equivalent to that of the wild-type yeast protein. A requirement for the vector was evidenced by its absence in all transformants that lost the lactate growth phenotype after propagation in nonselective medium. In contrast, the level of vector-specific message in single copy was equivalent to that of the endogenous ADC1 mRNA, but transformants exhibited no significant growth on lactate. Constructions having a small deletion or a mammalian intron within the rat cytochrome c coding region failed to support lactate-dependent growth, indicating that complementation depends upon proper translation of the correct rat coding sequence. Therefore, the rat polypeptide, when expressed at normal physiological levels, is recognized by the yeast machinery involved in the multiple steps required for the processing and transport of an active cytochrome c as well as its functional interaction with the respiratory apparatus.     

Imported mitochondrial proteins cytochrome b2 and cytochrome c1 are processed in two steps.

Cytochrome b2 of yeast is located in the space between the inner and outer mitochondrial membranes whereas cytochrome c1 is bound to the outer face of the mitochondrial inner membrane. Both proteins are made outside the mitochondria as larger precursors that are processed to their mature forms in two steps. In the first step, at least a segment of the precursor polypeptide chain penetrates into the mitochondrial matrix and is cleaved to an intermediate form by a matrix-localized soluble protease. This step requires an electrochemical gradient across the mitochondrial inner membrane. In the second step, the intermediate form is converted to the mature form. For cytochrome c1, this second step requires heme. Import of these two cytochromes thus involves a "detour" across the inner membrane.     

Exploring the proton pump and exit pathway for pumped protons in cytochrome ba3 from Thermus thermophilus

The heme-copper oxygen reductases are redox-driven proton pumps. In the current work, the effects of mutations in a proposed exit pathway for pumped protons are examined in the ba(3)-type oxygen reductase from Thermus thermophilus, leading from the propionates of heme a(3) to the interface between subunits I and II. Recent studies have proposed important roles for His376 and Asp372, both of which are hydrogen-bonded to propionate-A of heme a(3), and for Glu126(II) (subunit II), which is hydrogen-bonded to His376. Based on the current results, His376, Glu126(II), and Asp372 are not essential for either oxidase activity or proton pumping. In addition, Tyr133, which is hydrogen-bonded to propionate-D of heme a(3), was also shown not to be essential for function. However, two mutations of the residues hydrogen-bonded to propionate-A, Asp372Ile and His376Asn, retain high electron transfer activity and normal spectral features but, in different preparations, either do not pump protons or exhibit substantially diminished proton pumping. It is concluded that either propionate-A of heme a(3) or possibly the cluster of groups centered about the conserved water molecule that hydrogen-bonds to both propionates-A and -D of heme a(3) is a good candidate to be the proton loading site.