Structural and kinetic characterization of active-site histidine as a proton shuttle in catalysis by human carbonic anhydrase II

In the catalysis of the hydration of carbon dioxide and dehydration of bicarbonate by human carbonic anhydrase II (HCA II), a histidine residue (His64) shuttles protons between the zinc-bound solvent molecule and the bulk solution. To evaluate the effect of the position of the shuttle histidine and pH on proton shuttling, we have examined the catalysis and crystal structures of wild-type HCA II and two double mutants: H64A/N62H and H64A/N67H HCA II. His62 and His67 both have their side chains extending into the active-site cavity with distances from the zinc approximately equivalent to that of His64. Crystal structures were determined at pH 5.1-10.0, and the catalysis of the exchange of (18)O between CO(2) and water was assessed by mass spectrometry. Efficient proton shuttle exceeding a rate of 10(5) s(-)(1) was observed for histidine at positions 64 and 67; in contrast, relatively inefficient proton transfer at a rate near 10(3) s(-)(1) was observed for His62. The observation, in the crystal structures, of a completed hydrogen-bonded water chain between the histidine shuttle residue and the zinc-bound solvent does not appear to be required for efficient proton transfer. The data suggest that the number of intervening water molecules between the donor and acceptor supporting efficient proton transfer in HCA II is important, and furthermore suggest that a water bridge consisting of two intervening water molecules is consistent with efficient proton transfer.     

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.     

Kinetic analysis of multiple proton shuttles in the active site of human carbonic anhydrase

We have prepared a site-specific mutant of human carbonic anhydrase (HCA) II with histidine residues at positions 7 and 64 in the active site cavity. Using a different isozyme, we have placed histidine residues in HCA III at positions 64 and 67 and in another mutant at positions 64 and 7. Each of these histidine residues can act as a proton transfer group in catalysis when it is the only nonliganding histidine in the active site cavity, except His(7) in HCA III. Using an (18)O exchange method to measure rate constants for intramolecular proton transfer, we have found that inserting two histidine residues into the active site cavity of either isozyme II or III of carbonic anhydrase results in rates of proton transfer to the zinc-bound hydroxide that are antagonistic or suppressive with respect to the corresponding single mutants. The crystal structure of Y7H HCA II, which contains both His(7) and His(64) within the active site cavity, shows the conformation of the side chain of His(64) moved from its position in the wild type and hydrogen-bonded through an intervening water molecule with the side chain of His(7). This suggests a cause of decreased proton transfer in catalysis.     

Gaugement of the inner space of the apomyoglobin's heme binding site by a single free diffusing proton. I. Proton in the cavity.

Time resolved fluorimetry was employed to monitor the geminate recombination between proton and excited pyranine anion locked, together with less than 30 water molecules, inside the heme binding site of Apomyoglobin (sperm whale). The results were analyzed by a numerical reconstruction of the differential rate equation for time-dependent diffusion controlled reaction with radiating boundaries using N. Agmon's procedure (Huppert, Pines, and Agmon, 1990, J. Opt. Soc. Am. B., 7:1541-1550). The analysis of the curve provided the effective dielectric constant of the proton permeable space in the cavity and the diffusion coefficient of the proton. The electrostatic potential within the cavity was investigated by the equations given by Gilson et al. (1985, J. Mol. Biol., 183:503-516). According to this analysis the dielectric constant of the protein surrounding the site is epsilon prot < or = 6.5. The diffusion coefficient of the proton in the heme binding site of Apomyoglobin-pyranine complex is D = 4 x 10(-5) cm2/s. This value is approximately 50% of the diffusion coefficient of proton in water. The lower value indicates enhanced ordering of water in the cavity, a finding which is corroborated by a large negative enthropy of binding delta S0 = -46.6 cal.mole-1 deg-1. The capacity of a small cavity in a protein to retain a proton had been investigated through the mathematical reconstruction of the dynamics. It has been demonstrated that Coulombic attraction, as large as delta psi of energy coupling membrane, is insufficient to delay a free proton for a time frame comparable to the turnover time of protogenic sites.     

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.     

Properties of intramolecular proton transfer in carbonic anhydrase III.

We investigated the efficiency of glutamic acid 64 and aspartic acid 64 as proton donors to the zinc-bound hydroxide in a series of site-specific mutants of human carbonic anhydrase III (HCA III). Rate constants for this intramolecular proton transfer, a step in the catalyzed dehydration of bicarbonate, were determined from the proton-transfer-dependent rates of release of H2 18O from the enzyme measured by mass spectrometry. The free energy plots representing these rate constants could be fit by the Marcus rate theory, resulting in an intrinsic barrier for the proton transfer of deltaG0++ = 2.2 +/- 0.5 kcal/mol, and a work function or thermodynamic contribution to the free energy of reaction wr = 10.8 +/- 0.1 kcal/mol. These values are very similar in magnitude to the Marcus parameters describing intramolecular proton transfer from His64 and His67 to the zinc-bound hydroxide in mutants of HCA III. That result and the equivalent efficiency of Glu64 and Asp64 as proton donors in the catalysis by CA III demonstrate a lack of specificity in proton transfer from these sites, which is indirect evidence of a number of proton conduction pathways through different structures of intervening water chains. The dominance of the thermodynamic contribution or work function for all of these proton transfers is consistent with the view that formation and breaking of hydrogen bonds in such water chains is a limiting factor for proton translocation.     

Dynamics of the proton transfer reaction on the cytoplasmic surface of bacteriorhodopsin

The cytoplasmic surface of bacteriorhodopsin is characterized by a group of carboxylates that function as a proton attractive domain [Checover, S., Nachliel, E., Dencher, N. A., and Gutman, M. (1997) Biochemistry 36, 13919-13928]. To identify these carboxylates, we selectively mutated them into cysteine residues and monitored the effects of the dynamics of proton transfer between the bulk and the surface of the protein. The measurements were carried out without attachment of a pH-sensor to the cysteine residue, thus avoiding any structural perturbation and change in the surface charge caused by the attachment of a reporter group, and the protein was in its BR state. The purple membranes were suspended in an unbuffered solution of pyranine (8-hydroxypyrene-1,3,6-trisulfonate) and exposed to a train of 1000 laser pulses (2.1 mJ/pulse, lambda = 355 nm, at 10 Hz). The excitation of the dye ejected the hydroxyl's proton, and a few nanoseconds later, a pair of free protons and ground-state pyranine anion was formed. The experimental observation was the dynamics of the relaxation of the system to the prepulse state. The observed signals were reconstructed by a numeric method that replicates the chemical reactions proceeding in the perturbed space. The detailed reconstruction of the measured signal assigned the various proton-binding sites with rate constants for proton binding and proton exchange and the pK values. Comparison of the results obtained by the various mutants indicates that the dominant proton-binding cluster of the wild-type protein consists of D104, E161, and E234. The replacement of D104 or E161 with cysteine lowered the proton binding capacity of the cluster to approximately 60% of that of the native protein. The replacement of E234 with cysteine disrupted the structure of the cluster, causing the two remaining carboxylates to function as isolated residues that do not interact with each other. The possibility of proton transfer between monomers is discussed.     

Thermodynamic stability of water molecules in the bacteriorhodopsin proton channel: a molecular dynamics free energy perturbation study.

The proton transfer activity of the light-driven proton pump, bacteriorhodopsin (bR) in the photochemical cycle might imply internal water molecules. The free energy of inserting water molecules in specific sites along the bR transmembrane channel has been calculated using molecular dynamics simulations based on a microscopic model. The existence of internal hydration is related to the free energy change on transfer of a water molecule from bulk solvent into a specific binding site. Thermodynamic integration and perturbation methods were used to calculate free energies of hydration for each hydrated model from molecular dynamics simulations of the creation of water molecules into specific protein-binding sites. A rigorous statistical mechanical formulation allowing the calculation of the free energy of transfer of water molecules from the bulk to a protein cavity is used to estimate the probabilities of occupancy in the putative bR proton channel. The channel contains a region lined primarily by nonpolar side-chains. Nevertheless, the results indicate that the transfer of four water molecules from bulk water to this apparently hydrophobic region is thermodynamically permitted. The column forms a continuous hydrogen-bonded chain over 12 A between a proton donor, Asp 96, and the retinal Schiff base acceptor. The presence of two water molecules in direct hydrogen-bonding association with the Schiff base is found to be strongly favorable thermodynamically. The implications of these results for the mechanism of proton transfer in bR are discussed.     

Role of hydrophilic residues in proton transfer during catalysis by human carbonic anhydrase II

Catalysis by the zinc metalloenzyme human carbonic anhydrase II (HCA II) is limited in maximal velocity by proton transfer between His64 and the zinc-bound solvent molecule. Asn62 extends into the active site cavity of HCA II adjacent to His64 and has been shown to be one of several hydrophilic residues participating in a hydrogen-bonded solvent network within the active site. We compared several site-specific mutants of HCA II with replacements at position 62 (Ala, Val, Leu, Thr, and Asp). The efficiency of catalysis in the hydration of CO 2 for the resulting mutants has been characterized by (18)O exchange, and the structures of the mutants have been determined by X-ray crystallography to 1.5-1.7 A resolution. Each of these mutants maintained the ordered water structure observed by X-ray crystallography in the active site cavity of wild-type HCA II; hence, this water structure was not a variable in comparing with wild type the activities of mutants at residue 62. Crystal structures of wild-type and N62T HCA II showed both an inward and outward orientation of the side chain of His64; however, other mutants in this study showed predominantly inward (N62A, N62V, N62L) or predominantly outward (N62D) orientations of His64. A significant role of Asn62 in HCA II is to permit two conformations of the side chain of His64, the inward and outward, that contributes to maximal efficiency of proton transfer between the active site and solution. The site-specific mutant N62D had a mainly outward orientation of His64, yet the difference in p K a between the proton donor His64 and zinc-bound hydroxide was near zero, as in wild-type HCA II. The rate of proton transfer in catalysis by N62D HCA II was 5% that of wild type, showing that His64 mainly in the outward orientation is associated with inefficient proton transfer compared with His64 in wild type which shows both inward and outward orientations. These results emphasize the roles of the residues of the hydrophilic side of the active site cavity in maintaining efficient catalysis by carbonic anhydrase.     

The dynamics of proton transfer between adjacent sites.

The mechanism of proton transfer at the interface is the most prevalent reaction in the biosphere, yet its modeling at atomic level is still technically impossible. The difficulties emerge from the quantum mechanical nature of the proton, the modulation of the local electrostatic potential by the protein-water dielectric boundary and the formation of covalent bonds with proton binding sites whenever encounters take place. To circumvent some of these difficulties, and to identify the effect of the local electrostatic field, we present molecular dynamics simulations, where Na+ and Cl- ions diffuse at the surface of a small model protein, the S6 of the bacterial ribosome. The analysis reveals the presence of a detained state, where an ion is located for a relatively long period within the immediate environment of certain attractor residues. In the detained state the ion retains its ability to diffuse, yet the local field deters it from leaving to the bulk. When an ion is detained inside a Coulomb cage, it has a high probability to be transferred between nearby attractors, thus forming a mechanism similar to that responsible for the proton collecting antenna present on proton proteins.     

Coupling of light-induced electron transfer to proton uptake in photosynthesis

Light energy is transformed into chemical energy in photosynthesis by coupling a light-induced electron transfer to proton uptake. The resulting proton gradient drives ATP synthesis. In this study, we monitored the light-induced reactions in a 100-kDa photosynthetic protein from 30 ns to 35 s by FTIR difference spectroscopy. The results provide detailed mechanistic insights into the electron and proton transfer reactions of the QA to QB transition: reduction of QA in picoseconds induces protonation of histidines, probably of His126 and His128 in the H subunit at the entrance of the proton uptake channel, and of Asp210 in the L subunit inside the channel at 12 micros and 150 micros. This seems to be a prerequisite for the reduction of QB, mainly at 150 micros. QA- is reoxidized at 1.1 ms, and a proton is transferred from Asp210 to Glu212 in the L subunit, the proton donor to QB-. Notably, our data indicate that QB is not reduced directly by QA- but presumably through an intermediary electron donor.     

Tautomerism of histidine 64 associated with proton transfer in catalysis of carbonic anhydrase

The imidazole (15)N signals of histidine 64 (His(64)), involved in the catalytic function of human carbonic anhydrase II (hCAII), were assigned unambiguously. This was accomplished by incorporating the labeled histidine as probes for solution NMR analysis, with (15)N at ring-N(delta1) and N(epsilon2), (13)Cat ring-Cepsilon1, (13)C and (15)N at all carbon and nitrogen, or (15)N at the amide nitrogen and the labeled glycine with (13)C at the carbonyl carbon. Using the pH dependence of ring-(15)N signals and a comparison between experimental and simulated curves, we determined that the tautomeric equilibrium constant (K(T)) of His(64) is 1.0, which differs from that of other histidine residues. This unique value characterizes the imidazole nitrogen atoms of His(64) as both a general acid (a) and base (b): its epsilon2-nitrogen as (a) releases one proton into the bulk, whereas its delta1-nitrogen as (b) extracts another proton from a water molecule within the water bridge coupling to the zinc-bound water inside the cave. This accelerates the generation of zinc-bound hydroxide to react with the carbon dioxide. Releasing the productive bicarbonate ion from the inside separates the water bridge pathway, in which the next water molecules move into beside zinc ion. A new water molecule is supplied from the bulk to near the delta1-nitrogen of His(64). These reconstitute the water bridge. Based on these features, we suggest here a catalytic mechanism for hCAII: the tautomerization of His(64) can mediate the transfers of both protons and water molecules at a neutral pH with high efficiency, requiring no time- or energy-consuming processes.     

Structural and kinetic analysis of proton shuttle residues in the active site of human carbonic anhydrase III

We report the X-ray crystal structures and rate constants for proton transfer in site-specific mutants of human carbonic anhydrase III (HCA III) that place a histidine residue in the active-site cavity: K64H, R67H, and K64H-R67N HCA III. Prior evidence from the exchange of 18O between CO2 and water measured by mass spectrometry shows each mutant to have enhanced proton transfer in catalysis compared with wild-type HCA III. However, His64 in K64H and K64H-R67N HCA III have at most a capacity for proton transfer that is only 13% that of His64 in HCA II. This reduced rate in mutants of HCA III is associated with a constrained side-chain conformation of His64, which is oriented outward, away from the active-site zinc in the crystal structures. This conformation appears stabilized by a prominent pi stacking interaction of the imidazole ring of His64 with the indole ring of Trp5 in mutants of HCA III. This single orientation of His64 in K64H HCA III predominates also in a double mutant K64H-R67N HCA III, indicating that the positive charge of Arg67 does not influence the observed conformation of His64 in the crystal structure. Hence, the structures and catalytic activity of these mutants of HCA III containing His64 account only in small part for the lower activity of this isozyme compared with HCA II. His67 in R67H HCA III was also shown to be a proton shuttle residue, having a capacity for proton transfer that was approximately four times that of His64 in K64H HCA III. This is most likely due to its proximity and orientation inward towards the zinc-bound solvent. These results emphasize the significance of side chain orientation and range of available conformational states as characteristics of an efficient proton shuttle in carbonic anhydrase.     

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.     

Proton-collecting properties of bovine heart cytochrome C oxidase: kinetic and electrostatic analysis.

Proton-transfer reactions on the surface of bovine heart cytochrome c oxidase were investigated by combining a laser-induced proton-pulse technique with molecular modeling. The experimental approach simultaneously monitors the state of pyranine protonation in the bulk phase and that of a fluorescein indicator specifically attached to the native Cys(III-115) residue of subunit III of cytochrome oxidase. The reversible dynamics of the acid-base equilibration between the surface and the bulk phase were measured with submicrosecond time resolution and analyzed by numerical integration of coupled nonlinear differential rate equations. Kinetic analysis shows that carboxylates on the surface of the protein act as a proton-collecting antenna, which is able to rapidly transfer protons to nearby histidines that function as a local proton reservoir. These properties enable cytochrome oxidase to carry out its redox-linked proton translocation. Molecular modeling of the fluorescein-binding site indicates that, in addition to the covalent bond, the dye is anchored through a hydrogen bond to the hydroxyl moiety of Tyr(VII-50). The protonation of the dye is mediated through three residues that shuttle protons between the bulk and the dye. A correlation between the measured kinetic properties of the bound fluorescein and the different configurations of the dye allows us to predict the identity of the proton-binding sites in the fluorescein-binding domain.     

Proton transfer in a Thr200His mutant of human carbonic anhydrase II

Human carbonic anhydrase II (HCA II) has a histidine at position 64 (His64) that donates a proton to the zinc-bound hydroxide in catalysis of the dehydration of bicarbonate. To examine the effect of the histidine location on proton shuttling, His64 was replaced with Ala and Thr200 replaced with histidine (H64A-T200H HCAII), effectively relocating the proton shuttle residue 2 A closer to the zinc-bound hydroxide compared to wild type HCA II. The crystal structure of H64A-T200H HCA II at 1.8 A resolution shows the side chain of His200 directly hydrogen-bonded with the zinc-bound solvent. Different proton transfer processes were observed at pH 6 and at pH 8 during the catalytic hydration-dehydration cycle, measured by mass spectrometry as the depletion of 18O from C18O2 by H64A-T200H HCA II. The process at pH 6.0 is attributed to proton transfer between the side chain of His200 and the zinc-bound hydroxide, in analogy with proton transfer involving His64 in wild-type HCA II. At pH 8.0 it is attributed to proton transfer between bicarbonate and the zinc-bound hydroxide, as supported by the dependence of the rate of proton transfer on bicarbonate concentration and on solvent hydrogen isotope effects. This study establishes that a histidine directly hydrogen-bonded to the zinc-bound hydroxide, can adopt the correct distance geometry to support proton transfer     

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.     

Inhibition of proton transfer in cytochrome c oxidase by zinc ions: delayed proton uptake during oxygen reduction

We have investigated the effect of Zn ions on proton-transfer reactions in cytochrome c oxidase. In the absence of Zn(2+) the transition from the "peroxy" (P(R)) to the "ferryl" (F) intermediate has a time constant of approximately 100 micros and it is associated with proton transfer from the bulk solution with an intrinsic time constant of <100 micros, but rate limited by the P(R)-->F transition. While in the presence of 100 microM Zn(2+) the P(R)-->F transition was slowed by a factor of approximately 2, proton uptake from the bulk solution was impaired to a much greater extent. Instead, about two protons (one proton in the absence of Zn(2+)) were taken up during the next reaction step, i.e. the decay of F to the oxidized (O) enzyme with a time constant of approximately 2.5 ms. Thus, the results show that there is one proton available within the enzyme that can be used for oxygen reduction and confirm our previous observation that F can be formed without proton uptake from the bulk solution. No effect of Zn(2+) was observed with a mutant enzyme in which Asp(I-132), at the entry point of the D-pathway, was replaced by its non-protonatable analogue Asn. In addition, no effect of Zn(2+) was observed on the F-->O transition rate when measured in D(2)O, because in D(2)O, the transition is internally slowed to approximately 10 ms, which is already slower than with bound Zn(2+). Together with earlier results showing that both the P(R)-->F and F-->O transitions are associated with proton uptake through the D-pathway, the results from this study indicate that Zn(2+) binds to and blocks the entrance of the D-pathway.     

Effect of xenon binding to a hydrophobic cavity on the proton pumping cycle in bacteriorhodopsin

To understand the functional role of apolar cavities in bacteriorhodopsin, a light-driven proton pump found in Halobacterium salinarum, we investigated the crystal structure in pressurized xenon or krypton. Diffraction data from the P622 crystal showed that one Xe or Kr atom binds to a preexisting hydrophobic cavity buried between helices C and D, located at the same depth from the membrane surface as Asp96, a key residue in the proton uptake pathway. The occupation fraction of Xe or Kr was calculated as approximately 0.32 at a pressure of 1 MPa. In the unphotolyzed state, the binding of Xe or Kr caused no large deformation of the cavity. However, the proton pumping cycle was greatly perturbed when an aqueous suspension of purple membrane was pressurized with xenon gas; that is, the decay of the M state was accelerated significantly (~5 times at full occupancy), while the decay of an equilibrium state of N and O was slightly decelerated. A similar but much smaller perturbation in the reaction kinetics was observed upon pressurization with krypton gas. In a glycerol/water mixture, xenon-induced acceleration of M decay became less significant in proportion to the water activity. Together with the structure of the xenon-bound protein, these observations suggest that xenon binding helps water molecules permeate into apolar cavities in the proton uptake pathway, thereby accelerating the water-mediated proton transfer from Asp96 to the Schiff base.