doi:10.1016/j.jmb.2008.09.074 J. Mol. Biol. (2008) 384, 865–877 Available online at www.sciencedirect.com A D-Pathway Mutation Decouples the Paracoccus denitrificans Cytochrome c Oxidase by Altering the Side-Chain Orientation of a Distant Conserved Glutamate Katharina L. Dürr 1 ⁎, Juergen Koepke 2 , Petra Hellwig 3 , Hannelore Müller 2 , Heike Angerer 2 , Guohong Peng 2 , Elena Olkhova 2 , Oliver-Matthias H. Richter 1 , Bernd Ludwig 1,4 and Hartmut Michel 2,4 1 Department of Biochemistry, Molecular Genetics Group, Johann Wolfgang Goethe University, Max-von-Laue-Str. 9, D-60438 Frankfurt/Main, Germany 2 Department of Molecular Membrane Biology, Max Planck Institute of Biophysics, Max-von-Laue-Str. 3, D-60438 Frankfurt/Main, Germany 3 Institute of Biophysics, Johann Wolfgang Goethe University, Max-von-Laue-Str. 1, D-60438 Frankfurt/Main, Germany 4 Cluster of Excellence Frankfurt Macromolecular Complexes, Johann Wolfgang Goethe University, Max-von-Laue-Str. 3, D-60438 Frankfurt/Main, Germany Asparagine 131, located near the cytoplasmic entrance of the D-pathway in subunit I of the Paracoccus denitrificans aa3 cytochrome c oxidase, is a residue crucial for proton pumping. When replaced by an aspartate, the mutant enzyme is completely decoupled: while retaining full cytochrome c oxidation activity, it does not pump protons. The same phenotype is observed for two other substitutions at this position (N131E and N131C), whereas a conservative replacement by glutamine affects both activities of the enzyme. The N131D variant oxidase was crystallized and its structure was solved to 2.32-Å resolution, revealing no significant overall change in the protein structure when compared with the wild type (WT), except for an alternative orientation of the E278 side chain in addition to its WT conformation. Moreover, remarkable differences in the crystallographically resolved chain of water molecules in the D-pathway are found for the variant: four water molecules that are observed in the water chain between N131 and E278 in the WT structure are not visible in the variant, indicating a higher mobility of these water molecules. Electrochemically induced Fourier transform infrared difference spectra of decoupled mutants confirm that the protonation state of E278 is unaltered by these mutations but indicate a distinct perturbation in the hydrogen-bonding environment of this residue. Furthermore, they suggest that the carboxylate side chain of the N131D mutant is deprotonated. These findings are discussed in terms of their mechanistic implications for proton routing through the D-pathway of cytochrome c oxidase. © 2008 Elsevier Ltd. All rights reserved. Received 27 June 2008; received in revised form 28 August 2008; accepted 17 September 2008 Available online 9 October 2008 Edited by R. Huber Keywords: Proton pumping; proton gating; water chain; electron transfer; FTIR spectroscopy *Corresponding author. Max-Volmer-Laboratory for Biophysical Chemistry, Institute of Chemistry, Technical University of Berlin, Secr. PC 14, Strasse des 17. Juni 135, D-10623 Berlin, Germany. E-mail address: [email protected]. Present address: P. Hellwig, Institut de Chimie, UMR 7177, CNRS, Université Louis Pasteur, 4, rue Blaise Pascal, 67000 Strasbourg, France. Abbreviations used: COX, cytochrome c oxidase; WT, wild type; CCCP, carbonyl cyanide m-chlorophenylhydrazone; FTIR, Fourier transform infrared; SHE, standard hydrogen electrode; P side, positively charged aqueous side of the membrane; PLS, proton loading site; DM, n-dodecyl-β-D-maltoside. 0022-2836/$ - see front matter © 2008 Elsevier Ltd. All rights reserved. 866 Introduction Cytochrome c oxidase (COX) is a terminal member of the aerobic respiratory chain of mitochondria and many bacteria, including Paracoccus denitrificans and Rhodobacter sphaeroides. It catalyzes electron transfer from cytochrome c to molecular oxygen (dioxygen) and utilizes the free energy provided by this redox reaction to generate an electrochemical proton gradient across the inner mitochondrial and bacterial cytoplasmic membrane, respectively. During a full dioxygen reduction cycle, eight protons are taken up from the inside, four for water formation (“substrate protons”) and four for translocation across the membrane (“vectorial or pumped protons”).1 In aa3-type COXs, which also include the mitochondrial oxidase, four redox-active cofactors participate in electron transfer: CuA, the primary electron acceptor from cytochrome c; heme a; and the binuclear center consisting of CuB and heme a3, where binding and reduction of oxygen take place. At least two proton-conducting pathways, termed D-pathway and K-pathway (see Fig. 1), have been Fig. 1. Structures of subunits I and II of the four-subunit complex of the aa3 COX from P. denitrificans (Protein Data Bank code 1AR1) illustrating the two proton-conducting pathways of the enzyme: D-pathway (red) and K-pathway (green). A putative proton exit pathway is also indicated (black arrow). Functionally important amino acid side chains in the pathways (including N131) are represented as sticks. The VMD software was used for visualization.2 Structural Insights from a Decoupled COX Variant identified by analyzing both structural data3–8 and mutagenesis studies.9–20 These pathways connect the inner aqueous phase and the binuclear site. The initial concept that protons consumed in water formation at the active site use the K-pathway and translocated protons are transferred via the Dpathway3 could not be maintained because measurements of charge translocation21,22 and results from flow-flash experiments23,24 indicated that the K-pathway delivers the first one or two protons to the binuclear center during the reductive phase of the catalytic cycle only, with the remaining two or three substrate protons transported via the D-pathway during the “oxidative” part of the cycle (after the binding of molecular oxygen to the reduced binuclear center of COX). All pumped protons appear to use the D-pathway. Proton translocation in these pathways has been proposed to occur via hydrogen-bonded chains, so called “proton wires,”25–28 which include amino acid residues and bound water molecules. 29,30 According to the Grotthuss mechanism of proton transfer (reviewed in Refs. 26 and 31), an excess proton can travel along such a chain of hydrogen bonds when each non-hydrogen atom, usually an oxygen or a nitrogen, in the chain is a donor and an acceptor of a hydrogen bond, giving rise to a much higher rate of proton translocation compared to a simple diffusion process. The individual proton is just relayed from the donor to the acceptor, followed by a conformational reorganization. As a consequence of the observation that the Dpathway is used for pumped protons and substrate protons, a mechanism differentiating substrate protons from pumped protons (“gating”) in the D-pathway must operate, but its molecular mechanism remains unknown. Results from several studies3,32–47 indicate that the side chain of Glu278, located at the upper end of the D-pathway, may be the key element for gating. From Glu278, protons are funneled into two sites (see Fig. 1 for illustration), with one being the binuclear center and the other a yet unidentified protonatable cluster [often referred to as pump site X or proton loading site (PLS)] from which pumped protons are eventually expelled to the P side (positively charged aqueous side) of the membrane. The direction of proton transfer beyond Glu278 has been discussed in terms of a reorientation of proton-conducting water arrays controlled by the redox state-dependent electric field between heme a and the binuclear center.32,39 Several mutations that selectively abolish proton pumping have been identified in positions N13115,48,49 and N19915,50 (P. denitrificans numbering is used unless otherwise stated). Since they are located in a region of the D-pathway far below E278 (Fig. 1), they might a priori be expected to impair the uptake of both substrate and pumped protons, for example as reported for D124N.12–14,16 The selective loss of proton pumping in the former variants has therefore been attributed to impeding the branching function of E278 by a yet unknown mechanism. 867 Structural Insights from a Decoupled COX Variant The best characterized example of such a decoupled variant is N131D.15,48,51–54 The corresponding mutation of the homologous residue N139 in R. sphaeroides has been suggested to decouple the proton pump by increasing the apparent pKa value of E286 (E278 in P. denitrificans) in the PR state from 9.4 to 11,52 as concluded from pH level-dependent measurements of the rate for the PR → F transition, reflecting the protonation state of E286. Continuum electrostatic calculations yield still higher values for this variant.55,56 More recently, it has been reported that the R. sphaeroides decoupling mutation N207D (N199D in P. denitrificans) is correlated with an even higher shift of the E286 apparent pK.50,56 Since the restoration of the original charge distribution by the additional mutation D132N (D124N in P. denitrificans) at the entrance of the D-pathway was shown to restore proton pumping in the N139D (N131D in P. denitrificans) variant,57 researchers have suggested that introducing a charged side chain influences the glutamate side chain via long-range electrostatic interactions. However, the relatively long distance of about 20 Å between the two residues renders an electrostatic effect rather unlikely. Furthermore, continuum electrostatic calculations suggest that the effect of the introduced negative charge in the N131D variant on E278 is very small in terms of changing its pKa.55 Olsson and Warshel were able to calculate the effect of the N139D (N131D in P. denitrificans) mutation on proton pumping.54 They concluded from changes in the free energy surface for proton translocation of the variant that the electrostatic potential of water molecules below E286 (E278 in P. denitrificans) is altered, thereby stopping the flow of protons to the P side and trapping the proton in the binuclear center. More recently, in a replacement of N139 by the neutral amino acid Thr, 49 the apparent pKa of E286 was shown to be shifted in the opposite direction, again supporting the view that the observed pKa changes have no electrostatic origin but rather reflect a possible E286 side-chain reorientation caused by the mutations. Despite all experimental and computational efforts to elucidate the mechanism of decoupling in these enzyme variants, it is presently still unclear how these mutations lead to a selective loss of proton pumping and whether this phenomenon requires a negatively charged group in the center of the D-pathway. In this study, we systematically replaced the N131 residue with different amino acids in order to evaluate its role in proton pumping. Interestingly, replacement by strongly acidic residues, such as aspartate and glutamate, leads to selective loss of proton pumping. In addition, an exchange by the weakly acidic cysteine results in a decoupled enzyme. Redox Fourier transform infrared (FTIR) spectroscopy was used to monitor the effects of mutations introduced at position 131 on the protonation state of residue E278. The crystal structure of the N131D variant determined at 2.32 Å resolution surprisingly reveals an additional E278 conformation along with changes in the positions and occupancies of the crystallographically resolved water molecules in the D-pathway, which, taken together, appear responsible for the decoupled phenotype of this variant. Results Cytochrome c oxidation activity and proton pumping The wild type (WT) and all mutant enzymes, histidine tagged at the C-terminus of subunit I, were purified using a Ni–nitrilotriacetic acid affinity column. As judged from SDS-gel electrophoresis (data not given), the isolated COX complexes showed a normal four-subunit composition, with all mutated I subunits migrating identically with their WT counterpart. UV/VIS spectroscopic features were indistinguishable from those obtained for the WT, with heme/protein ratios varying between 14 and 17 nmol heme a/mg. We first characterized the mutant enzymes with respect to their steady-state cytochrome c oxidation activity (listed in Table 1). The activity of the N131D variant is, within experimental error, identical to the WT, as reported earlier.15,48 Two further replacements of N131 by Glu and Cys affected the turnover number only marginally (Table 1), thus also displaying cytochrome c oxidation activities again comparable with the WT enzyme. In contrast, a substitution of the Asn by the longer glutamine side chain diminished the steady-state activity by almost 50%. When hydrophobic amino acid residues are introduced in this position, the turnover number of the enzyme decreases drastically, resulting in residual cytochrome c oxidation activity of 11% and 3% for the N131A and N131V variants, respectively. A similarly substantial loss in turnover rate was also observed for the N131Y variant, which retains 6% of the WT activity. Proton pump stoichiometries were determined with the use of a stopped-flow spectrometric approach after reconstitution of the purified COXs into Table 1. Catalytic activities and proton pump stoichiometries of purified P. denitrificans aa3 COX variants in comparison with the WT activity Oxidase type Cytochrome c oxidation activity (%) Proton translocation (H+/e−) WT N131D N131E N131C N131Q N131A N131V N131Y 100.0 ± 12.3 114.0 ± 16.7 77.9 ± 14.9 86.4 ± 11.4 52.2 ± 4.1 10.7 ± 1.0 2.6 ± 0.2 6.2 ± 0.9 1.04 ± 0.15 0.09 ± 0.02 0.12 ± 0.02 0.12 ± 0.02 0.40 ± 0.09 0.04 ± 0.01 n.d. n.d. One hundred percent activity corresponds to a turnover number of 458 electrons s− 1. Data are expressed as the mean ± SE of at least three independent experiments. n.d. indicates not determined. 868 Fig. 2. Changes in phenol red absorbance followed at 555.6 nm (isosbestic point of cytochrome c) in the presence and in the absence of the protonic uncoupler CCCP for the WT and several mutant enzymes. Proton pump stoichiometries obtained by an exponential fitting procedure are listed in Table 1. proteoliposomes. Figure 2 illustrates the transient changes in phenol red absorbance recorded after mixing the proteoliposomes with reduced cytochrome c for WT and several mutant COXs. A rapid exponential decrease of the phenol red absorbance for the WT enzyme indicates transient acidification of the extravesicular medium. In the presence of the protonophore carbonyl cyanide mchlorophenylhydrazone (CCCP), a net alkalization is the result of the consumption of protons in water formation. With the WT enzyme pumping one Structural Insights from a Decoupled COX Variant proton per transferred electron, the phenol red absorbance changes in the absence and in the presence of CCCP should be identical in absolute numbers. In fact, after exponential fitting of the absorbance changes, we obtained a H+/e− ratio of 1.04 for the WT enzyme. In contrast, none of our mutant enzymes reached this proton pump activity (see Table 1). For example, the N131Q variant resulted in reduced proton pumping with a stoichiometry of about 0.4 H+/e−. Three mutants, N131D, N131C, and N131E, although retaining full cytochrome c oxidation activity, display a proton pump stoichiometry of approximately 0.1 H+/e− and may thus be safely classified as “ideally decoupled” mutants. In contrast, the pump stoichiometry of 0.04 H+ /e− experimentally determined for the N131A variant is difficult to assess: while this mutation may indeed lead to a defect in pumping, it cannot be excluded that its substantially reduced cytochrome c oxidation rate results in experimental difficulties in the system used here. Since respiratory control ratios of the COX vesicles determined separately were between 4.1 and 7.5 for the variants and approximately 10.0 for the WT enzyme (data not shown), none of the mutations produces a leak for protons across the membrane. FTIR spectroscopic characterization of uncoupled variants Figure 3A presents the oxidized-minus-reduced FTIR difference spectra of WT, N131D, N131C, and N199D mutant enzymes for a potential step from − 0.292 to 0.708 V at pH 7.0. Overall, the difference spectra of the various mutant enzymes are similar in shape, indicating that no major structural change occurs upon mutation. The signature previously assigned to the reorganization of the protonated Fig. 3. (A) Oxidized-minus-reduced FTIR difference spectra of WT and N131D, N131C, and N199D mutant COXs from P. denitrificans for a potential step from −0.5 to 0.5 V versus Ag/AgCl (corresponding to a potential step from −0.292 to 0.708 V SHE′). (B) Oxidized-minus-reduced FTIR difference spectra of WT (dashed dotted line), N131D (continuous line), and N131C (dashed line) COXs from P. denitrificans for a potential step from −0.5 to 0.5 V versus Ag/AgCl (corresponding to a potential step from −0.292 to 0.708 V SHE′). (C) Oxidized-minus-reduced FTIR difference spectra of WT (dasheddotted line) and N131C variant (continuous line) COXs from P. denitrificans, with samples equilibrated at pH 9.2, for a potential step from − 0.5 to 0.5 V versus Ag/AgCl (corresponding to a potential step from − 0.292 to 0.708 V SHE′). Structural Insights from a Decoupled COX Variant form of Glu278 58,59 is present for all variants analyzed; a small upward shift of 4 cm− 1 indicates a minor variation in the hydrogen-bonding environment for the reduced form. In the oxidized form, shifts of about 1–2 cm− 1 occur for all variants, but this observation may not be significant since the resolution of the spectra is 4 cm− 1. Some variations can be found between 1580 and 1500 cm− 1 for the N131D mutant enzyme, which is shown in direct comparison with the WT enzyme and the N131C variant enzyme in Fig. 3B. Interestingly, a broad signal at 1586 cm− 1 is perturbed together with signals around 1420–1390 cm− 1. These spectral ranges are characteristic for the signals of the respective asymmetric and symmetric modes of deprotonated acidic side chains, respectively. Since the modes are absent in the N131C variant enzyme, they may be assigned to originate from the introduced aspartic acid in the N131D variant. We suggest that its carboxylate is deprotonated and reorganizes upon redox reaction. Spectra at pH 9.2 have been obtained and are presented in Fig. 3C for the WT and the N131C variant in order to probe a possible effect of the mutations on the pH level dependence of the redox-dependent behavior. Furthermore, in this study, major spectral features remained essentially unchanged in both samples. We note that the broad positive mode at 1439 cm− 1 arises from the B = O vibration of the borate buffer. For both samples, WT and N131C, the presence of difference signals at 1746 and 1734 cm− 1 in the spectra at pH 9.2 reveals that Glu278 is protonated in the reduced and oxidized forms. Again, a small shift of the signals by approximately 4 cm− 1 is seen, obviously arising from a small variation in the hydrogenbonding environment. X-ray structure of the N131D variant at 2.32 Å resolution When comparing the atomic coordinates of the N131D variant structure (resolved to 2.32 Å) to the ones of the recently refined WT structure (Koepke et al., unpublished results) truncated to 2.29 Å resolution (see Materials and Methods), no significant difference in the overall protein structure is detectable (RMSD = 0.498 Å). The backbone and side-chain conformations seem to be virtually identical with the WT structure. However, two features distinguish the variant structure from WT: (i) Two electron densities are seen for the side chain of the highly conserved residue E278, indicating two side-chain orientations: One (shown in orange in Fig. 4) is identical to the E278 orientation observed in the WT structure (in magenta in Fig. 4), and is also found in other COX structures, such as those from bovine heart mitochondria8,60 and R. sphaeroides.6 In this downward orientation, the E278 side chain is within hydrogen-bonding distance to a water molecule (Wat551), which participates in a 869 Fig. 4. Superposition of the P. denitrificans N131D variant (carbon atoms in yellow) with the WT (magenta) structure. Hydrogen bonds between water molecules of the WT accounting for a water chain along the D-pathway are represented by green dashed lines, with their respective lengths given in Å. These hydrogen bonds were restrained during the final refinement cycles to 2.8 Å. The electron density of the variant structure around water molecules accounting for the D-pathway is given in green wire-frame representation at the level of 0.2σ. A difference Fourier density between variant and WT structures was calculated and is presented as blue (positive density) and red (negative) wire frames at the level of ±2σ. The electron density for the water molecules 465, 899, 962, 968, and 969 is missing in the variant structure, indicated by a negative difference density (red) and in addition by magenta labels of these water positions. The missing water molecules reflect a higher flexibility of the D-pathway water chain in the variant structure. The side chain of Glu278 was refined in two orientations. Thus, one orientation of this residue is marked by carbon atoms shown in orange. hydrogen-bonding network important for proton transfer in the D-pathway. This conformation of E278 might be required for taking up protons from the D-pathway, thus being often referred to as the “input” conformation of this residue. In the other conformational state revealed by the present N131D variant structure, the E278 side chain points upward (in 870 Structural Insights from a Decoupled COX Variant yellow in Fig. 4). A similar configuration of the corresponding residue was observed in the Xray structure of the variant E286Q6 and in WT COX from R. sphaeroides at pH 10.0 (as cited in Refs. 61 and 62). According to previous theoretical studies on COX,29,33,39,47,63 such a conformational state of E278 is considered as a “proton release” configuration from which a “loaded” proton is transferred either to the binuclear center or to a “proton loading/pump site” near the heme a3 propionates. The routing of protons further on from this “output” configuration depends on the relative energy barriers, which are presumably modulated by the redox state of the oxygen intermediates at the active site, as well as on the presence of a transient pathway for proton transfer, which may exist for very short periods only because of rapid fluctuations of water molecules.29 (ii) Distinct changes in the positions of water molecules are observed in the N131D structure, in the vicinity of the D-pathway: In the cavity between residue 131 and E278, several water molecules can be resolved from the electron density of the variant (Fig. 4, green wire frame) and WT (data not shown) structures, forming a continuous hydrogen-bonded water chain connecting the two residues. These water molecules are represented by spheres in Fig. 4, shown in magenta for the WT structure and in red for the N131D variant structure. Notably, five water molecules are missing in the variant structure, which becomes obvious when the difference Fourier electron density between the variant and the WT electron density is considered (red and blue wire frames in Fig. 4, representing negative and positive difference densities at a level of ±2σ, respectively). Distinct negative difference densities are observed below E278 (missing Wat969 and Wat899), close to residue 131 (missing Wat962 and Wat968), and near the entrance of the D-pathway (missing Wat465). For comparison, in the WT structure, the electron densities for these water molecules near N131 are approximately 0.6σ and more than 1σ for those close to E278. To exclude the possibility that the observed differences arise from the different resolutions of the two relevant structures, we calculated both applying the same reflections (see Materials and Methods). The remaining minor difference in resolution is due to the differences in unit cell dimensions of the data sets. Discussion In this study, further replacements in the N131 position of the Paracoccus COX were analyzed and characterized by FTIR spectroscopy, and the N131D variant was crystallized and its structure was determined at 2.32 Å. An interesting correlation is found between its defects in proton pumping and structural alterations in the mutant enzyme. E278 conformation is altered in the N131D decoupled variant The central finding in this work is an additional density for the E278 side chain observed in the N131D crystal structure. Considering the generally accepted role of this conserved glutamate as a potential redox-controlled switch directing protons either to the binuclear center or to a PLS around the heme a3 propionates, the structural alteration found for the N131D variant appears to be of particular importance for the observed selective loss of proton pumping. Whereas the WT (downward) configuration is also found in X-ray COX structures from other species,6,8 the simultaneous existence of both sidechain orientations of this glutamate as observed here in the N131D mutant enzyme has never been seen directly before. On the other hand, it has already been suggested in the first description of a COX structure3 and is in agreement with results from redox-FTIR spectroscopy.58 In addition, simulation calculations have provided evidence for the existence of (several) additional glutamate side-chain conformations.33,39,40,47,63 Our own full-scale molecular dynamics simulations29 of COX in the fully oxidized state have indicated that the side chain of E278 moves into the upward orientation (see Refs. 40 and 55) if it is deprotonated. Interestingly, this orientation was also found in the R. sphaeroides WT structure at pH 10.0 (unpublished results by Gennis & Brzezinski, cited in Refs. 61 and 62). These findings suggest that the alternative “up” orientation may be populated only transiently in specific steps of the regular reaction cycle and thus cannot be revealed in static X-ray structures of the WT enzyme. The additionally observed E278 “up” (Gluup) conformation of the N131D variant structure reflects a higher occupancy of this transient state that is apparently caused by the mutation. According to results from a recent molecular dynamics study of the corresponding E242 (bovine heart mitochondria COX numbering) side-chain rotational isomerization,63 this transient conformational “up” state is supposed to be extremely vulnerable to leakage of protons from the PLS back to E242. In the bovine WT COX, a rapid (∼ 1 ps), highly exergonic downward flip of the deprotonated E242 side chain (Glu− up) to the other conformation (Glu−down) is assumed to be essential for “valve” function, thus ensuring that protons stored at the PLS are only ejected to the P side.64 The additional “up” conformation revealed in the Paracoccus N131D variant structure seems to indicate that this crucial fast transition is impeded as a consequence of the mutation, which would compromise the E278 valve function, thus explaining its decoupled phenotype. Alternatively, the altered side-chain orientation of E278 may affect its proton funneling properties: The rotational mobility of the E278 carboxylate in the variant may be reduced and, consequently, the E278 Structural Insights from a Decoupled COX Variant side chain is preferentially “locked” in one position, unable to supply protons to the pump site at all but nevertheless allowing an ample number of protons to reach the binuclear site for oxygen reduction. With the aforementioned assumption that the altered E278 orientation now delivers all protons taken up from the D-pathway to the binuclear site instead of discriminating between pumped and substrate protons in mind, we may even explain the increased cytochrome c oxidation activity reported for the N139D variant from R. sphaeroides.48 Observed effects on E278 in decoupled variants are probably not of electrostatic nature Considering the distance of at least 18 Å, it is far from obvious how the E278 conformational change observed for the P. denitrificans N131D variant in this work or the increased E286 pKa reported for the R. sphaeroides N139D variant may be linked to the site of mutation. An electrostatic effect of the ionized aspartate side chain introduced by the mutation in position N139 was proposed by Namslauer et al.65 Similarly, an electrostatically derived pKa shift of E286 was also assumed to be responsible for the observed decoupling of the variant N207D in R. sphaeroides.50 These pKa increases were computationally confirmed for both ionic variants in a recent continuum electrostatic calculation.56 Moreover, the coupled phenotype in the charge-shift double variant N139D/D132N was attributed to a restoration of the E286 pKa,57 thus corroborating the idea that the effects of the decoupled variants are of electrostatic nature. In our work, the deprotonated state of N131D was confirmed by redox-FTIR spectroscopy, in support of this explanation. On the other hand, the spectra of decoupled mutants did not reveal a different protonation state for the E278 side chain reflecting possible pKa alterations. However, it must be emphasized that the shifted pKa values observed for the decoupled R. sphaeroides mutants are “apparent” ones that are characteristic only of the transient PR state49,50,65—such pKa alterations are therefore most likely not revealed by the redoxFTIR method applied here. According to our calculations,55 the charge–charge interaction energies between the two acidic residues E278 and N131D are quite low, mainly due to the long distance of 18 Å. Very recently, an electrostatic influence was considered more likely for charged residues introduced closer to E278 (e.g., at a distance of 7 Å, such as S197D in R. sphaeroides20). Furthermore, our findings show that not only acidic replacement of N131 by Asp or Glu but also the presumably neutral side-chain substitution by Cys results in decoupling of the COX redoxdriven proton pump. According to our electrostatic calculations, which predict a pKa between 10.7 and 22.2 depending on the dielectric constant applied,55 deprotonation of the N131C side chain, causing a change in the pKa of E278 by electrostatic interaction, is rather unlikely. Therefore, the decoupled 871 phenotype of at least this particular variant must be explained by another mechanism, similarly to the recently characterized N139T variant from R. sphaeroides, in which the loss of proton pumping also cannot be attributed to electrostatic effects due to the neutral Thr replacement.49 Distorted water structure in the D-pathway is characteristic of decoupled variants Molecular dynamics simulations indicate that a continuous chain of water molecules, connecting D124 up to E278, is not present in the D-pathway.29,30 Accordingly, in several X-ray structures, 6 the crystallographically resolved water molecules form a continuous hydrogen-bonded proton wire only between E278 and N131, which is connected to D124 via a single water molecule (see also Fig. 4). It was proposed that the side chains of N131 and another conserved asparagine (N113) in its direct vicinity are required to maintain the tight connectivity between these two water chains.53 However, one has to keep in mind that asparagines in the given structure cannot be part of a proton-connecting hydrogen-bonded network. With the side-chain carbonyl oxygen only being a hydrogen-bond acceptor, they interrupt the “proton wire” and block proton transfer. Therefore, they may offer a potential gating function, controlling the access of solvent protons further up the D-pathway. A reorientation of these asparagine side chains is necessary to allow the formation of an effective proton-transferring hydrogenbonded chain from D124 up to E278. These conclusions are in agreement with the results of free energy profile calculations for excess protons in the D-pathway.53 With the aforementioned considerations, it is interesting to note the reduced number of observable water molecules in the D-pathway of the N131D variant structure presented here when compared with the WT. We interpret this as an indication of a higher mobility of these water molecules since large cavities in protein structures without any crystallographically defined water molecules are often filled with disordered water molecules.66,67 Changes are most prominent in the immediate vicinity of the mutated N131D side chain, at the entrance of the D-pathway near D124, and around E278. Such changes in the water structure around E286 were also postulated for the decoupled N139D and N207D variants from R. sphaeroides,68 since the redox-FTIR spectra of these two variants exhibited a slight shift of the E286 signature, indicating an alteration of the chain of water molecules running from the site of mutation up to E286. A very similar effect is seen in the corresponding FTIR spectrum for the N131C variant presented in this work (Fig. 3B and C), suggesting a common mechanistic explanation for the decoupling observed in all such variants (i.e., a perturbation of the position or orientation of water molecules within the D-pathway). 872 Correct hydrogen bonding may be crucial to stabilize the proton-conducting water chain The asparagine side chain can form hydrogen bonds as a donor and as an acceptor. This property may be crucial to the abovementioned functions of the three asparagines. In contrast, the mutated N131D side chain in its deprotonated form, as evidenced by our FTIR experiments, can only be a hydrogen acceptor, unable to provide hydrogen bonds to Asn113 and Wat972 (see Fig. 4). As a result of the mutation introduced here, the polarity of the hydrogen-bonded chain is changed and the hydrogen-bond pattern is disturbed. These effects may be responsible for the observed perturbation of the water structure in the middle of the D-pathway and be further propagated up to E278 (see below). The notion that the decoupled phenotype of the N131D mutant is rather a consequence of the perturbed hydrogen-bonding capability of the mutated aspartate side chain and not due to its ionic state is supported by the newly identified N131C (this work) and N139T49 (R. sphaeroides) variants, in which uncharged side chains are also less suited for hydrogen bonding (as donors of only a single hydrogen bond instead of two hydrogen bonds), resulting in a decoupled phenotype as well. However, any conclusive explanation as to how a proton can be transferred from Asp124/Wat622 via Asn/Asp131 to Wat972 (see Fig. 4) on the opposite side of the asparagine cluster is still missing. A protonated Asp side chain could transfer a proton via a side-chain rotation, as also indicated by the results of a theoretical study53 that predicted an accelerated proton translocation by a neutral Asp side chain compared with a negatively charged one. However, one has to keep in mind that assuming a pKa of 5 for Asp131, it would be protonated in a rapid dynamic equilibrium for 0.5% of the time at pH 7.0. Whenever it is protonated, the side chain may rotate and deliver a proton to Wat972 and thus lead to an acceleration of proton transfer from the inner side to E278 compared with the WT. Actually, the question on whether the N131D mutation leads to a deceleration or an acceleration of proton transfer is far from being settled. Indeed, results of measurements of the transmembrane charge separation for the F-to-O transition with the homologous N139D variant from R. sphaeroides suggest that the mutation leads to an acceleration of the rate (τ) of the slowest proton uptake phase via the D-pathway from 1.5 to 0.6 ms.51 In addition, the fact that the decoupled turnover of the homologous N139D variant in R. sphaeroides is more than 400% of the coupled turnover of the WT enzyme48 is more easily reconciled with an enhanced proton transfer through the Dpathway than with a diminished one (but see below and Ref. 69 for an alternative explanation for the increased N139D turnover rates). Provided that the changes in the water mobility and the hydrogen-bonding pattern actually affect proton translocation in the D-pathway, still the question arises as to why, selectively, proton pumping but not Structural Insights from a Decoupled COX Variant water formation at the active site is impaired. On the basis of the two variant structure-derived key observations, the perturbed E278 side-chain position (s) and the changes in the proton-wire water structure, we envisage two possible explanations: (i) Precise timing of proton delivery may be more demanding for proton pumping than for water formation (“kinetic gating”) A changed proton conduction due to the altered water structure and hydrogen bonding in the Dpathway may not deliver protons within a distinct time window required for proton pumping. Assuming that a less precise timing is necessary for substrate protons consumed at the binuclear center for water formation, a reduction in proton transfer rate would selectively affect proton pumping and not the steady-state cytochrome c oxidation activity. This is in line with the “kinetic gating mechanism” proposed by Popovic and Stuchebrukhov.70 They suggested that E278 may be connected to the PLS and the active site by two separate proton-transporting water networks offering different proton conduction rates. It is assumed that the “faster” one delivers pumped protons to the PLS, whereas the chemical protons are provided by the “slower” one, thus ensuring that a proton is preloaded into the pump site before the driving redox event (protonation of the reduced oxygen intermediates at the active site by substrate protons) occurs. Since both networks are supplied with protons via the Dpathway, a moderately decreased proton translocation rate, possibly caused by the D-pathway water rearrangement, might become rate limiting only for the fast proton-conducting network, thereby decoupling the proton pump. Moreover, this explanation is also in agreement with a suggestion recently provided by Wikström and Verkhovsky.69 They assumed that a slowed proton translocation caused by the mutated N131D side chain may delay reprotonation of E278, which decouples the pump by lowering the barrier for proton transfer from the “pump site” back to E278 (see also below). In their model, this would result in a bypass of the slowest step of the proton pumping cycle and explain even the enhanced steady-state cytochrome c oxidation activity of the N139D variant (R. sphaeroides). Furthermore, hydrophobic replacements of the N131 side chain, which cannot provide any stabilizing hydrogen bonds at all, are expected to cause even more pronounced perturbations of the water structure. Consequently, the proton translocation rate would be slowed substantially and the delivery of substrate protons via the mutated Dpathway eventually becomes rate limiting even for oxygen chemistry at the binuclear site, thus also affecting steady-state turnover. This is consistent with the experimentally observed drastically reduced cytochrome c oxidation activity of the hydrophobic variants N131A and N131V or the N131Y variant (Table 1), with its limited ability to form hydrogen bonds. 873 Structural Insights from a Decoupled COX Variant (ii) A lowered rate of proton conductance in the Dpathway impairs the E278 switch (by shifting the conformational equilibrium of the E278 side-chain orientation) It was proposed in a recent molecular dynamics simulation of the E242 (corresponding to E278) sidechain rotational isomerization63 that a lowered rate of proton conductance in the D-pathway may raise the kinetic barrier for the Glu−down-to-GluHdown transition (reprotonation of the anionic Glu−down via the D-pathway). Consequently, the Glu−down state accumulates, which in turn increases the occupancy of the Glu−up state. This seems reasonable since the additional E278 conformation revealed by the N131D variant structure actually supports such an increased population of the Glu−up state. As already outlined above, this state is assumed to be vulnerable to leakage of protons from the pump site back to E278, thus explaining the selective loss of proton pumping of the decoupled variants. Both the kinetic (i) and conformational (ii) arguments may also be linked to each other and thus contribute to various extents to the observed phenotype. (iii) Caused by local environment changes in the variant enzyme exhibiting an alternative E278 orientation, the pKa of E278 may be shifted, thus rendering the side chain unsuitable to deliver protons to the pump site. Finally, with the N131C mutant enzyme phenotype largely identical with the corresponding N131D mutant COX, former explanations invoking electrostatic effects appear less substantiated. Materials and Methods Site-directed mutagenesis Site-directed mutagenesis was performed according to the QuikChange site-directed mutagenesis protocol (Stratagene). All mutations introduced into the ctaDII gene encoding subunit I15,16 were confirmed by DNA sequencing. Mutated ctaDII genes were subcloned into pKH48, a derivative of pUP3915 carrying a C-terminal six-histidine affinity tag. Bacterial growth, protein purification, and crystallization Conclusions The X-ray structure of a decoupled variant (N131D) of the P. denitrificans COX provides evidence for the simultaneous population of an alternative conformational state of the E278 side chain considered to be of prime importance for the routing of “chemical” and “pumped” protons, acting as a kinetic valve in the WT COX to prevent proton leakage from the P side. In addition, several distinct differences are seen for the arrangement of water molecules in the proton-conveying D-pathway of the variant. These structural findings suggest that the distorted water structure in the D-pathway and/or an impeded branching function of the E278 side chain in the variant may be responsible for the observed phenotype, explained by one, singly, or by a combination of the following mechanistic scenarios: (i) A shifted conformational equilibrium of the two E278 side-chain orientations impairs either (a) its function as a switch separating pumped and substrate protons delivered by the D-pathway or (b) its recently proposed “valve” function, resulting in leakage of pumped protons from the PLS back to E278, which selectively inhibits proton pumping without affecting the routing of substrate protons to the binuclear site. (ii) An impeded proton transfer rate through the D-pathway, due to changes in water positions observed in the N131D variant structure, is not compatible with the required time regime for proton pumping in the variants. pKH48 plasmids carrying mutated subunit I genes were conjugated into the P. denitrificans recipient strain AO1, lacking functional aa3- and cbb3-type COXs.16 Bacterial cells were grown at 32 °C to an optical density at 600 nm N 3 in succinate medium16,71 supplemented with 25 μg/ml of streptomycin. Membranes isolated from these cells were solubilized in n-dodecyl-β-D-maltoside (DM) and applied to a Ni–nitrilotriacetic acid affinity column (QIAGEN), which allows purification of the four-subunit COX complex in a single-step procedure.72 Isolated COX complexes were characterized for their subunit composition with the use of SDS-gel electrophoresis, by recording their visible redox difference spectra and by determining their heme a/protein ratios. For crystallization purposes, WT and N131D mutant COXs were expressed in P. denitrificans strain AO1 using construct pUP3916 lacking a histidine tag. Accordingly, the two-subunit COX was purified via Fv antibody fragment 7E2C50S73 and crystallized as described previously.3,4 Determination of enzymatic activities of isolated enzymes Enzymatic activity was determined as previously described74 with 20 μM reduced horse heart cytochrome c (Sigma) using a reaction buffer containing 20 mM Tris– HCl, pH 7.5, 20 mM KCl, 1 mM ethylenediaminetetraacetic acid, and 0.2 g/l of DM. The assay was performed at 550 nm in a Hitachi U-3000 spectrophotometer. Reconstitution of purified COX into liposomes and determination of proton pumping Asolectin (phospatidylcholine, type II-S, Sigma) and cholate were purified as described elsewhere.75 A total of 40 mg/ml of purified asolectin was resuspended in 100 mM Hepes–KOH, pH 7.3, 10 mM KCl, and 2% cholate and stirred at 4 °C until all particles were dissolved. 874 Subsequently, the solution was sonicated at intervals of 30 s (Branson Sonifier II 250, 30% duty cycle) until the solution appeared translucent (both steps were carried out under nitrogen atmosphere). After a short centrifugation (6000g, 15 min, 4 °C) to remove particulate material, purified COX previously eluted from a Q-Sepharose column by 100 mM Hepes–KOH, 500 mM KCl, and 0.15 g/l of DM was added to a final concentration of 4 μM. After a sequence of dialysis steps,76 the mixture was centrifuged again (6000g, 15 min, 4 °C) and the supernatant was used for proton pump measurements. Stopped-flow measurements recording the absorbance changes of the pH-sensitive dye phenol red photometrically were carried out essentially as described in Ref. 77 using a stopped-flow spectrometer (Hi-Tech Scientific SF-61). A suspension containing 0.4 μM COX in proteoliposomes, 60 μM phenol red, and 10 μM valinomycin was prepared in the last dialysis buffer, and reduced horse heart cytochrome c at a final concentration of 200 μM was equilibrated in the same buffer. After adjusting the pH levels of both solutions to 7.3, solutions were filled into 2.5- and 0.25-ml syringes of the stopped-flow spectrometer, respectively. The 10:1 ratio of syringes was chosen to avoid mixing artefacts.76,78 The absorbance change of phenol red was monitored at 25 °C and 555.6 nm, which was determined to be the isosbestic point for cytochrome c under the experimental conditions. For determination of the decoupled rates, the procedure was repeated after adding CCCP (final concentration = 10 μM) to the solution containing the proteoliposomes. Electrochemistry The ultra-thin-layer spectroelectrochemical cell for the UV/VIS and IR was used as previously described.79 Sufficient transmission in the range of 1800 to 1000 cm− 1, even in the region of strong water absorbance around 1645 cm− 1, was achieved with the cell path length set to 6–8 μm. The gold-grid working electrode was chemically modified with a 2 mM cysteamine solution as reported before.58 In order to accelerate the redox reaction, we added 16 mediators as reported in Ref. 58 (except nmethylphenazoniummethosulfate and n-ethylphenazoniumsulfate) to a final concentration of 45 μM each. At this concentration, and with the cell path length below 10 μm, no spectral contribution from the mediators in the VIS and IR ranges could be detected in control experiments with samples lacking the protein, except for the PO modes of the phosphate buffer between 1200 and 1000 cm− 1. Potentials quoted with the data refer to the Ag/AgCl/3 M KCl reference electrode. The potential step from − 0.5 to + 0.5 V applied here therefore corresponds to a potential step from −0.292 to 0.708 V SHE′ (standard hydrogen electrode). Electrochemistry samples were equilibrated in 100 mM phosphate buffer, pH 7.0, or borate buffer, pH 9.2, 100 mM KCl, and 0.15% DM each. FTIR spectroscopy FTIR and UV/VIS difference spectra as a function of the applied potential were obtained simultaneously from the same sample with a setup combining an IR beam from an interferometer (modified IFS 25, Bruker, Germany) for the range of 4000–1000 cm− 1 and a dispersive spectrometer Structural Insights from a Decoupled COX Variant for that of 400–900 nm. Electrochemically induced difference spectra were recorded and processed as described in Ref. 58. X-ray data collection, processing, and refinement The crystals were cryoprotected with 25% (v/v) glycerol and flash frozen in gaseous cryo-stream cooled by liquid nitrogen. X-ray diffraction data were collected on synchrotron beamline X10SA of the Swiss Light Source in Villigen, Switzerland. The collected data set was indexed and processed with the program XDS80 to a resolution of 2.32 Å. Data collection statistics are listed in Table 2. Recently, the structure of the cryo-cooled recombinant WT of the two-subunit COX from P. denitrificans has been refined (Koepke et al., unpublished results). Both data sets were loaded into a single mtz file using the CCP4 program CAD to truncate the native data set to exactly the same reflections used for the variant structure.81 Writing the data with MTZ2VARIOUS to an ASCII reflection file by ignoring the MISS command, controlling the missing reflection flag, leads to a file containing only entries that are common to both data sets. Subsequently, the ASCII file was reread with F2MTZ back into an mtz file for further use in the CCP4 suite of programs.81 Refinement in Refmac582 could be started directly from the WT structure, with the side chain of residue 131 changed according to the mutation to an aspartate. The structure factors were calculated from the measured intensities employing TRUNCATE of the CCP4 suite of programs. Between each refinement round, 2Fo − Fc and Fo − Fc electron density maps were inspected using the graphics program XtalView.83 Water molecules were added to the protein model at peaks N 3σ in the Fo − Fc difference density map, when the geometry was suitable for hydrogen bounding. In the membrane region, detergent molecules have been fitted to difference density peaks Table 2. Data collection statistics Data set 1AR1 Species Unit cell (Å) a 93.53 b 151.04 c 156.70 Space group Resolution (Å)a 2.7 7.4 Rsym (%)a a 2.05 Multiplicity Completeness 98.4 (%)a I/σ(I)a BWilson 23.5 (20.1) Rfree (R) (%) RMSD Bond (Å) Angle (°) Solvent 63 molecules Water 54 9 LDAOb c LMT WT N131D P. denitrificans 83.40 84.54 150.47 151.40 157.19 157.66 P212121 2.29 (2.4–2.29) 2.32 (2.4–2.32) 11.4 (35.9) 7.7 (39.0) 4.9 (4.8) 10.6 (8.7) 99.1 (98.0) 98.8 (97.0) 17.0 (3.5) 31.42 27.7 (21.4) 19.1 (3.9) 46.81 24.2 (20.5) 0.028 2.704 579 0.027 2.488 396 555 10 14 375 9 12 a Numbers in parentheses are values for the highest-resolution shell. b Lauryl dimethylamine oxide. c DM. Structural Insights from a Decoupled COX Variant instead. Since DM has been exchanged against lauryl dimethylamine oxide during purification, both detergent molecules were found. 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