Probing of the substrate binding domain of lactose permease by a proton pulse

The lactose permease of Escherichia coli coupled proton transfer across the bacterial inner membrane with the uptake of beta-galactosides. In the present study we have used the cysteine-less C148 mutant that was selectively labeled by fluorescein maleimide on the C148 residue, which is an active component of the substrate transporting cavity. Measurements of the protonation dynamics of the bound pH indicator in the time resolved domain allowed us to probe the binding site by a free diffusing proton. The measured signal was reconstructed by numeric integration of differential rate equations that comply with the detailed balance principle and account for all proton transfer reactions taking place in the reaction mixture. This analysis yields the rate constants and pK values of all residues participating in the fast proton transfer reaction between the bulk and the protein's surface, revealing the exposed residues that react with free protons in a diffusion controlled reaction and how they transfer protons among themselves. The magnitudes of these rate constants were finally evaluated by comparison with the rate predicted by the Debye-Smoluchowski equation. The analysis of the kinetic and pK values indicated that the protein-fluorescein adduct assumes two conformation states. One is dominant above pH 7.4, while the other exists only below 7.1. In the high pH range, the enzyme assumes a constrained configuration and the rate constant of the reaction of a free diffusing proton with the bound dye is 10 times slower than a diffusion controlled reaction. In this state, the carboxylate moiety of residue E126 is in close proximity to the dye and exchanges a proton with it at a very fast rate. Below pH 7.1, the substrate binding domain is in a relaxed configuration and freely accessed by bulk protons, and the rate of proton exchange between the dye and E126 is 100,000 times slower. The relevance of these observations to the catalytic cycle is discussed.     

Solvent proton relaxation studies of cytochrome c oxidase solutions

The interaction of solvent water protons with the bound paramagnetic metal ions of beef heart cytochrome c oxidase has been examined. The observed proton relaxation rates of enzyme solutions had a negative temperature dependence, indicating a rapid exchange between solvent protons in the coordination sphere of the metal ions and bulk solvent. An analysis of the dependence of the proton relaxation rate on the observation frequency indicated that the correlation time, which modulates the interaction between solvent protons and the unpaired electrons on the metal ions, is due to the electron spin relaxation time of the heme irons of cytochrome c oxidase. This means that at least one of the hemes is exposed to solvent. The proton relaxation rate of the oxidized enzyme was found to be sensitive to changes in ionic strength and to changes in the spin states of the metal ions. Heme a3 was found to be relatively inaccessible to bulk solvent. Partial reduction of the enzyme caused a slight increase in the relaxation rate, which may be due to a change in the antiferromagnetic coupling between two of the bound paramagnetic centers. Further reduction resulted in a decreased relaxation rate, and the fully reduced enzyme was no longer sensitive to changes in ionic strength. The binding of cytochrome c to cytochrome c oxidase had little effect on the proton relaxation rates of oxidized cytochrome oxidase indicating that cytochrome c binding has little effect on solvent accessibility to the metal ion sites.     

Relationship of proton release at the extracellular surface to deprotonation of the schiff base in the bacteriorhodopsin photocycle.

The surface potential of purple membranes and the release of protons during the bacteriorhodopsin photocycle have been studied with the covalently linked pH indicator dye, fluorescein. The titration of acidic lipids appears to cause the surface potential to be pH-dependent and causes other deviations from ideal behavior. If these anomalies are neglected, the appearance of protons can be followed by measuring the absorption change of fluorescein bound to various residues at the extracellular surface. Contrary to widely held assumption, the activation enthalpies of kinetic components, deuterium isotope effects in the time constants, and the consequences of the D85E, F208R, and D212N mutations demonstrate a lack of direct correlation between proton transfer from the buried retinal Schiff base to D85 and proton release at the surface. Depending on conditions and residue replacements, the proton release can occur at any time between the protonation of D85 and the recovery of the initial state. We conclude that once D85 is protonated the proton release at the extracellular protein surface is essentially independent of the chromophore reactions that follow. This finding is consistent with the recently suggested version of the alternating access mechanism of bacteriorhodopsin, in which the change of the accessibility of the Schiff base is to and away from D85 rather than to and away from the extracellular membrane surface.     

Bacteriorhodopsin in ice. Accelerated proton transfer from the purple membrane surface

The photocycle and the proton pumping kinetics of bacteriorhodopsin, as well as the transfer rate of protons from the membrane surface into the aqueous bulk phase were examined for purple membranes in water and ice. In water, the optical pH indicator pyranine residing in the aqueous bulk phase monitors the H(+)-release later than the pH indicator fluorescein covalently linked to the extracellular surface of BR. In the frozen state, however, pyranine responds to the ejected H+ as fast as fluorescein attached to BR, demonstrating that the surface/bulk transfer is in ice no longer rate limiting. The pumped H+ appears at the extracellular surface during the transition of the photocycle intermediate L550 to the intermediate M412. The Arrhenius plot of the M formation rate suggests that the proton is translocated through the protein via an ice-like structure.     

The mechanism of proton transfer between adjacent sites on the molecular surface

The surface of a protein, or a membrane, is spotted with a multitude of proton binding sites, some of which are only few A apart. When a proton is released from one site, it propagates through the water by a random walk under the bias of the local electrostatic potential determined by the distribution of the charges on the protein. Eventually, the released protons are dispersed in the bulk, but during the first few nanoseconds after the dissociation, the protons can be trapped by encounter with nearby acceptor sites. While the study of this reaction on the surface of a protein suffers from experimental and theoretical difficulties, it can be investigated with simple model compounds like derivatives of fluorescein. In the present study, we evaluate the mechanism of proton transfer reactions that proceed, preferentially, inside the Coulomb cage of the dye molecules. Kinetic analysis of the measured dynamics reveals the role of the dimension of the Coulomb cage on the efficiency of the reaction and how the ordering of the water molecules by the dye affects the kinetic isotope effect.     

Interplay between local protein interactions and water bridging of a proton antenna carboxylate cluster

Proteins that bind protons at cell membrane interfaces often expose to the bulk clusters of carboxylate and histidine sidechains that capture protons transiently and, in proton transporters, deliver protons to an internal site. The protonation-coupled dynamics of bulk-exposed carboxylate clusters, also known as proton antennas, is poorly described. An essential open question is how water-mediated bridges between sidechains of the cluster respond to protonation change and facilitate transient proton storage. To address this question, here I studied the protonation-coupled dynamics at the proton-binding antenna of PsbO, a small extrinsinc subunit of the photosystem II complex, with atomistic molecular dynamics simulations and systematic graph-based analyses of dynamic protein and protein-water hydrogen-bond networks. The protonation of specific carboxylate groups is found to impact the dynamics of their local protein-water hydrogen-bond clusters. Regardless of the protonation state considered for PsbO, carboxylate pairs that can sample direct hydrogen bonding, or bridge via short hydrogen-bonded water chains, anchor to nearby basic or polar protein sidechains. As a result, carboxylic sidechains of the hypothesized antenna cluster are part of dynamic hydrogen bond networks that may rearrange rapidly when the protonation changes.     

Subsecond proton-hole propagation in bacteriorhodopsin

The dynamics of proton transfer between the surface of purple membrane and the aqueous bulk have recently been investigated by the Laser Induced Proton Pulse Method. Following a Delta-function release of protons to the bulk, the system was seen to regain its state of equilibrium within a few hundreds of microseconds. These measurements set the time frame for the relaxation of any state of acid-base disequilibrium between the bacteriorhodopsin's surface and the bulk. It was also deduced that the released protons react with the various proton binding within less than 10 micro s. In the present study, we monitored the photocycle and the proton-cycle of photo-excited bacteriorhodopsin, in the absence of added buffer, and calculated the proton balance between the Schiff base and the bulk phase in a time-resolved mode. It was noticed that the late phase of the M decay (beyond 1 ms) is characterized by a slow (subsecond) relaxation of disequilibrium, where the Schiff base is already reprotonated but the pyranine still retains protons. Thus, it appears that the protonation of D96 is a slow rate-limiting process that generates a "proton hole" in the cytoplasmic section of the protein. The velocity of the hole propagation is modulated by the ionic strength of the solution and by selective replacements of charged residues on the interhelical loops of the protein, at domains that seems to be remote from the intraprotein proton conduction trajectory.     

The mechanism of proton transfer between adjacent sites on the molecular surface

The surface of a protein, or a membrane, is spotted with a multitude of proton binding sites, some of which are only few Å apart. When a proton is released from one site, it propagates through the water by a random walk under the bias of the local electrostatic potential determined by the distribution of the charges on the protein. Eventually, the released protons are dispersed in the bulk, but during the first few nanoseconds after the dissociation, the protons can be trapped by encounter with nearby acceptor sites. While the study of this reaction on the surface of a protein suffers from experimental and theoretical difficulties, it can be investigated with simple model compounds like derivatives of fluorescein. In the present study, we evaluate the mechanism of proton transfer reactions that proceed, preferentially, inside the Coulomb cage of the dye molecules. Kinetic analysis of the measured dynamics reveals the role of the dimension of the Coulomb cage on the efficiency of the reaction and how the ordering of the water molecules by the dye affects the kinetic isotope effect.     

Intramolecular proton-transfer reactions in a membrane-bound proton pump: the effect of pH on the peroxy to ferryl transition in cytochrome c oxidase

In the membrane-bound redox-driven proton pump cytochrome c oxidase, electron- and proton-transfer reactions must be coupled, which requires controlled modulation of the kinetic and/or thermodynamic properties of proton-transfer reactions through the membrane-spanning part of the protein. In this study we have investigated proton-transfer reactions through a pathway that is used for the transfer of both substrate and pumped protons in cytochrome c oxidase from Rhodobacter sphaeroides. Specifically, we focus on the formation of the so-called F intermediate, which is rate limited by an internal proton-transfer reaction from a possible branching point in the pathway, at a glutamic-acid residue (E(I-286)), to the binuclear center. We have also studied the reprotonation of E(I-286) from the bulk solution. Evaluation of the data in terms of a model presented in this work gives a rate of internal proton transfer from E(I-286) to the proton acceptor at the catalytic site of 1.1 x 10(4) s(-1). The apparent pK(a) of the donor (E(I-286)), determined from the pH dependence of the F-formation kinetics, was found to be 9.4, while the pK(a) of the proton acceptor at the catalytic site is likely to be > or = 2.5 pH units higher. In the pH range up to pH 10 the proton equilibrium between the bulk solution and E(I-286) was much faster than 10(4) s(-1), while in the pH range above pH 10 the proton uptake from solution is rate limiting for the overall reaction. The apparent second-order rate constant for proton transfer from the bulk solution to E(I-286) is >10(13) M(-1) s(-1), which indicates that the proton uptake is assisted by a local buffer consisting of protonatable residues at the protein surface.     

Protons @ interfaces: implications for biological energy conversion

The review focuses on the anisotropy of proton transfer at the surface of biological membranes. We consider (i) the data from "pulsed" experiments, where light-triggered enzymes capture or eject protons at the membrane surface, (ii) the electrostatic properties of water at charged interfaces, and (iii) the specific structural attributes of proton-translocating enzymes. The pulsed experiments revealed that proton exchange between the membrane surface and the bulk aqueous phase takes as much as about 1 ms, but could be accelerated by added mobile pH-buffers. Since the accelerating capacity of the latter decreased with the increase in their electric charge, it was concluded that the membrane surface is separated from the bulk aqueous phase by a barrier of electrostatic nature. The barrier could arise owing to the water polarization at the negatively charged membrane surface. The barrier height depends linearly on the charge of penetrating ions; for protons, it has been estimated as about 0.12 eV. While the proton exchange between the surface and the bulk aqueous phase is retarded by the interfacial barrier, the proton diffusion along the membrane, between neighboring enzymes, takes only microseconds. The proton spreading over the membrane is facilitated by the hydrogen-bonded networks at the surface. The membrane-buried layers of these networks can eventually serve as a storage/buffer for protons (proton sponges). As the proton equilibration between the surface and the bulk aqueous phase is slower than the lateral proton diffusion between the "sources" and "sinks", the proton activity at the membrane surface, as sensed by the energy transducing enzymes at steady state, might deviate from that measured in the adjoining water phase. This trait should increase the driving force for ATP synthesis, especially in the case of alkaliphilic bacteria.     

Proton binding to biological membranes

Biological membranes contain proton-binding moieties. A laser-induced proton pulse was used to characterize the proton-binding properties of bacterioopsin-containing membranes and of sarcoplasmic reticulum. Different protonation and deprotonation processes occurred. The liberation of protons from pyranine dye and the protonation of the membranes were independent of temperature; the reprotonation of pyranine and proton release from the membranes were temperature dependent. In the cases of membrane-free and membrane-containing systems, the activation enthalpies and entropies were calculated from the decay rates. The activation enthalpy of 16 kJ/mol for reprotonation of pyranine in membrane-free solution is characteristic for a diffusion-controlled process. The value for the membrane-containing systems was nearly double, suggesting that the buffering moieties of the membrane surfaces strongly bind the protons, raising the activation enthalpies. This is possibly an effect of the Coulomb cages formed from closely located proton acceptor sites. The activation entropies were positive in all cases.     

Oxygen and proton pathways in cytochrome c oxidase

Cytochrome c oxidase is a redox-driven proton pump, which couples the reduction of oxygen to water to the translocation of protons across the membrane. The recently solved x-ray structures of cytochrome c oxidase permit molecular dynamics simulations of the underlying transport processes. To eventually establish the proton pump mechanism, we investigate the transport of the substrates, oxygen and protons, through the enzyme. Molecular dynamics simulations of oxygen diffusion through the protein reveal a well-defined pathway to the oxygen-binding site starting at a hydrophobic cavity near the membrane-exposed surface of subunit I, close to the interface to subunit III. A large number of water sites are predicted within the protein, which could play an essential role for the transfer of protons in cytochrome c oxidase. The water molecules form two channels along which protons can enter from the cytoplasmic (matrix) side of the protein and reach the binuclear center. A possible pumping mechanism is proposed that involves a shuttling motion of a glutamic acid side chain, which could then transfer a proton to a propionate group of heme α₃. Proteins 30:100–107, 1998. © 1998 Wiley-Liss, Inc.     

Protons @ interfaces: Implications for biological energy conversion

The review focuses on the anisotropy of proton transfer at the surface of biological membranes. We consider (i) the data from “pulsed” experiments, where light-triggered enzymes capture or eject protons at the membrane surface, (ii) the electrostatic properties of water at charged interfaces, and (iii) the specific structural attributes of proton-translocating enzymes. The pulsed experiments revealed that proton exchange between the membrane surface and the bulk aqueous phase takes as much as about 1 ms, but could be accelerated by added mobile pH-buffers. Since the accelerating capacity of the latter decreased with the increase in their electric charge, it was concluded that the membrane surface is separated from the bulk aqueous phase by a barrier of electrostatic nature. The barrier could arise owing to the water polarization at the negatively charged membrane surface. The barrier height depends linearly on the charge of penetrating ions; for protons, it has been estimated as about 0.12 eV. While the proton exchange between the surface and the bulk aqueous phase is retarded by the interfacial barrier, the proton diffusion along the membrane, between neighboring enzymes, takes only microseconds. The proton spreading over the membrane is facilitated by the hydrogen-bonded networks at the surface. The membrane-buried layers of these networks can eventually serve as a storage/buffer for protons (proton sponges). As the proton equilibration between the surface and the bulk aqueous phase is slower than the lateral proton diffusion between the “sources” and “sinks”, the proton activity at the membrane surface, as sensed by the energy transducing enzymes at steady state, might deviate from that measured in the adjoining water phase. This trait should increase the driving force for ATP synthesis, especially in the case of alkaliphilic bacteria.     

Accessibility of the cytochrome a heme in cytochrome c oxidase to exchangeable protons

The comparison of the resonance Raman spectrum of cytochrome a2+ from cytochrome oxidase in deuterated buffers to that in protonated buffers reveals many lines that have different frequency or intensity. Some of the frequency differences are very large, e.g. on the order of 10 cm-1. From these differences in the Raman spectra, we infer that the heme pocket is readily accessible to protons and that labile groups are either on the heme or interact strongly with it. These data suggest the possibility of direct participation in proton translocation and/or oxygen protonation by the heme of cytochrome a.     

Proton transport via the membrane surface

Some proton pumps, such as cytochrome c oxidase (C(c)O), translocate protons across biological membranes at a rate that considerably exceeds the rate of proton transport to the entrance of the proton-conducting channel via bulk diffusion. This effect is usually ascribed to a proton-collecting antenna surrounding the channel entrance. In this paper, we consider a realistic phenomenological model of such an antenna. In our model, a homogeneous membrane surface, which can mediate proton diffusion toward the channel entrance, is populated with protolytic groups that are in dynamic equilibrium with the solution. Equations that describe coupled surface-bulk proton diffusion are derived and analyzed. A general expression for the rate constant of proton transport via such a coupled surface-bulk diffusion mechanism is obtained. A rigorous criterion is formulated of when proton diffusion along the surface enhances the transport. The enhancement factor is found to depend on the ratio of the surface and bulk diffusional constants, pK(a) values of surface protolytic groups, and their concentration. A capture radius for a proton on the surface and an effective size of the antenna are found. The theory also predicts the effective distance that a proton can migrate on the membrane surface between a source (such as CcO) and a sink (such as ATP synthase) without fully equilibrating with the bulk. In pure aqueous solutions, protons can travel over long distances (microns). In buffered solutions, the travel distance is much shorter (nanometers); still the enhancement effect of the surface diffusion on the proton flow to a target on the surface can be tens to hundreds at physiological buffer concentrations. These results are discussed in a general context of chemiosmotic theory.     

Stopped-flow studies of cytochrome oxidase reconstituted into liposomes: proton pumping and control of activity

The transient kinetics of proton pumping and the electron transfer properties of cytochrome oxidase inserted into small unilamellar vesicles have been investigated by stopped-flow spectrophotometry. In the presence of valinomycin, proton pumping and cytochrome c oxidation by cytochrome oxidase are synchronous up to rate constants of approximately 9 sec-1. Moreover, the enzyme depleted of subunit III ("three-less oxidase") was also shown to pump protons, although with a significantly smaller stoichiometry. Thus, subunit III is not the only (or even the main) proton channel, although it may be involved in the regulation of activity. The kinetics of cytochrome c oxidation by COV in the absence and in the presence of ionophores have been investigated. Analysis of the time course of the process in the transient and steady state phases indicates that the onset of control by the electrochemical gradient follows the transfer of four electrons, i.e., one complete turnover of the oxidase. Two possible alternative interpretations for the control of the turnover phase are presented and discussed.     

A role for subunit III in proton uptake into the D pathway and a possible proton exit pathway in Rhodobacter sphaeroides cytochrome c oxidase

Protons are transferred from the inner surface of cytochrome c oxidase to the active site by the D and K pathways, as well as from the D pathway to the outer surface by a largely undefined proton exit route. Alteration of the initial proton acceptor of the D pathway, D132, to alanine has previously been shown to greatly inhibit oxidase turnover and slow proton uptake into the D pathway. Here it is shown that the removal of subunit III restores a substantial rate of O(2) reduction to D132A. Presumably an alternative proton acceptor for the D pathway becomes active in the absence of subunit III and D132. Thus, in the absence of subunit III cytochrome oxidase shows greater flexibility in terms of proton entry into the D pathway. In the presence of DeltaPsi and DeltapH, turnover of the wild-type oxidase or D132A is slower in the absence of subunit III. Comparison of the turnover rates of subunit III-depleted wild-type oxidase to those of the zinc-inhibited wild-type oxidase containing subunit III, both reconstituted into vesicles, leads to the hypothesis that the absence of subunit III inhibits the ability of the normal proton exit pathway to take up protons from the outside in the presence of DeltaPsi and DeltapH. Thus, subunit III appears to affect the transfer of protons from both the inner and outer surfaces of cytochrome oxidase, perhaps accounting for the long-observed lower efficiency of proton pumping by the subunit III-depleted oxidase.     

The mechanism of transmembrane delta muH+ generation in mitochondria by cytochrome c oxidase.

In rat liver mitochondria treated with rotenone, N-ethylmaleimide or oligomycin the expected alkalinization caused by proton consumption for aerobic oxidation of ferrocyanide was delayed with respect to ferrocyanide oxidation, unless carbonyl cyanide p-trifluoromethoxyphenylhydrazone was present. 2. When valinomycin or valinomycin plus antimycin were also present, ferricyanide, produced by oxidation of ferrocyanide, was re-reduced by hydrogenated endogenous reductants. Under these circumstances the expected net proton consumption caused by ferrocyanide oxidation was preceded by transient acidification. It is shown that re-reduction of formed ferricyanide and proton release derive from rotenone- and antimycin-resistant oxidation of endogenous reductants through the proton-translocating segments of the respiratory chain on the substrate side of cytochrome c. The number of protons released per electron flowing to ferricyanide varied, depending on the experimental conditions, from 3.6 to 1.5. 3. The antimycin-insensitive re-reduction of ferricyanide and proton release from mitochondria were strongly depressed by 2-n-heptyl-4-hydroxyquinoline N-oxide. This shows that the ferricyanide formed accepts electrons passing through the protonmotive segments of the respiratory chain at the level of cytochrome c and/or redox components of the cytochrome b-c1 complex situated on the oxygen side of the antimycin-inhibition site. Dibromothymoquinone depressed and duroquinol enhanced, in the presence of antimycin, the proton-release process induced by ferrocyanide respiration. Both quinones enhanced the rate of scalar proton production associated with ferrocyanide respiration, but lowered the number of protons released per electron flowing to the ferricyanide formed. 4. Net proton consumption caused by aerobic oxidation of exogenous ferrocytochrome c by antimycin-supplemented bovine heart mitochondria was preceded by scalar proton release, which was included in the stoicheiometry of 1 proton consumed per mol of ferrocytochrome c oxidized. This scalar proton production was associated with transition of cytochrome c from the reduced to the oxidized form and not to electron flow along cytochrome c oxidase. 5. It is concluded that cytochrome c oxidase only mediates vectorial electron flow from cytochrome c at the outer side to protons that enter the oxidase from the matrix side of the membrane. In addition to this consumption of protons the oxidase does not mediate vectorial proton translocation.     

Cooperativity and flexibility of the protonmotive activity of mitochondrial respiratory chain

Functional and structural data are reviewed which provide evidence that proton pumping in cytochrome c oxidase is associated with extended allosteric cooperativity involving the four redox centers in the enzyme . Data are also summarized showing that the H+/e- stoichiometry for proton pumping in the cytochrome span of the mitochondrial respiratory chain is flexible. The DeltapH component of the bulk-phase membrane electrochemical proton gradient exerts a decoupling effect on the proton pump of both the bc1 complex and cytochrome c oxidase. A slip in the pumping efficiency of the latter is also caused by high electron pressure. The mechanistic and physiological implications of proton-pump slips are examined. The easiness with which bulk phase DeltapH causes, at least above a threshold level, decoupling of proton pumping indicates that for active oxidative phosphorylation efficient protonic coupling between redox complexes and ATP synthase takes place at the membrane surface, likely in cristae, without significant formation of delocalized DeltamuH+. A role of slips in modulating oxygen free radical production by the respiratory chain and the mitochondrial pathway of apoptosis is discussed.     

Proton translocation by a native and subunit III-depleted cytochrome c oxidase reconstituted into phospholipid vesicles. Use of fluorescein-phosphatidylethanolamine as an intravesicular pH indicator

The existence of a proton pump associated with bovine cytochrome c oxidase (EC 1.9.3.1) has over the last few years been a matter of considerable dispute. In an attempt to resolve some of the problems with the measuring system we have synthesized fluorescein-phosphatidylethanolamine which when reconstituted with cytochrome c oxidase into phospholipid vesicles provided a reliable indicator of the intravesicular pH. It was observed that cytochrome c oxidase catalyzed the abstraction of almost 2 protons from the intravesicular medium/molecule of ferrocytochrome c oxidized. In parallel experiments whereby the extravesicular pH was measured with an electrode it was found that the enzyme appeared to be responsible for the appearance of almost 1.0 proton/molecule of ferrocytochrome c oxidized. Taken together these data unequivocally demonstrate that cytochrome c oxidase behaves as a proton pump. Furthermore, the other proton which was abstracted is believed to be used for the process of the reduction of oxygen. Similar experiments were performed with a cytochrome c oxidase preparation which was devoid of subunit III. Under these circumstances the enzyme appeared to be unable to translocate protons across the vesicular membrane but was competent to abstract protons from the intravesicular medium for the reduction of oxygen.