Proton transport by phosphate diffusion--a mechanism of facilitated CO2 transfer

We have measured CO2 fluxes across phosphate solutions at different carbonic anhydrase concentrations, bicarbonate concentration gradients, phosphate concentrations, and mobilities. Temperature was 22-25 degrees C, the pH of the phosphate solutions was 7.0-7.3. We found that under physiological conditions of pH and pCO2 a facilitated diffusion of CO2 occurs in addition to free diffusion when (a) sufficient carbonic anhydrase is present, and (b) a concentration gradient of HCO3- is established along with a pCO2 gradient, and (c) the phosphate buffer has a mobility comparable to that of bicarbonate. When the phosphate was immobilized by attaching 0.25-mm-long cellulose particles, no facilitation of CO2 diffusion was detectable. A mechanism of facilitated CO2 diffusion in phosphate solutions analogous to that in albumin solutions was proposed on the basis of these findings: bicarbonate diffusion together with a facilitated proton transport by phosphate diffusion. A mathematical model of this mechanism was formulated. The CO2 fluxed predicted by the model agree quantitatively with the experimentally determined fluxes. It is concluded that a highly effective proton transport mechanism acts in solutions of mobile phosphate buffers. By this mechanism; CO2 transfer may be increased up to fivefold and proton transfer may be increased to 10,000-fold.     

Gaugement of the inner space of the apomyoglobin's heme binding site by a single free diffusing proton. II. Interaction with a bulk proton.

The reaction mechanism and the dynamic aspects of protonation of a defined moiety located inside an aqueous cavity in a protein were monitored by time resolved spectroscopy using the pyranine apomyoglobin complex as a model (Shimoni, Tsfadia, Nachliel, and Gutman, 1993, Biophys. J. 64:472-479). The reaction was synchronized by a short laser pulse and the reprotonation of the ground state pyranine anion (phi O-) was monitored, in the microsecond time scale, by its transient absorption at 457 nm. The observed signal was reconstructed by a numeric solution of nonlinear, coupled differential equations which account for the direct reaction of phi O- with bulk proton and by proton transfer from the nearby amino acids: His 64, Asp 44, Asp 60, and Glu 59. A unique combination of rate constant was obtained which quantitates the contribution of each pathway to the overall relaxation process. In the first phase of the dynamics phi O- abstracts a proton from the nearby protonated histidine. The bulk proton interacts preferentially with the cluster of three carboxylates and immediately shuttled to the deprotonated histidine. The high proximity of the reactive groups and the strong electrostatic forces operating inside the heme binding cavity render the rate of proton transfer in the site ultrafast.     

Calculated protein and proton motions coupled to electron transfer: electron transfer from QA- to QB in bacterial photosynthetic reaction centers.

Reaction centers from Rhodobacter sphaeroides were subjected to Monte Carlo sampling to determine the Boltzmann distribution of side-chain ionization states and positions and buried water orientation and site occupancy. Changing the oxidation states of the bacteriochlorophyll dimer electron donor (P) and primary (QA) and secondary (QB) quinone electron acceptors allows preparation of the ground (all neutral), P+QA-, P+QB-, P0QA-, and P0QB- states. The calculated proton binding going from ground to other oxidation states and the free energy of electron transfer from QA-QB to form QAQB- (DeltaGAB) compare well with experiment from pH 5 to pH 11. At pH 7 DeltaGAB is measured as -65 meV and calculated to be -80 meV. With fixed protein positions as in standard electrostatic calculations, DeltaGAB is +170 meV. At pH 7 approximately 0.2 H+/protein is bound on QA reduction. On electron transfer to QB there is little additional proton uptake, but shifts in side chain protonation and position occur throughout the protein. Waters in channels leading from QB to the surface change site occupancy and orientation. A cluster of acids (GluL212, AspL210, and L213) and SerL223 near QB play important roles. A simplified view shows this cluster with a single negative charge (on AspL213 with a hydrogen bond to SerL233) in the ground state. In the QB- state the cluster still has one negative charge, now on the more distant AspL210. AspL213 and SerL223 move so SerL223 can hydrogen bond to QB-. These rearrangements plus other changes throughout the protein make the reaction energetically favorable.     

Kinetics and mechanism of the acid transition of the active site in plastocyanin

Exchange on the microsecond time scale between the protonated and deprotonated forms of His92 in the copper site of reduced plastocyanin from the cyanobacteria Anabaena variabilis was monitored using 15N NMR relaxation measurements. On the basis of the dependence of the kinetics on pH and phosphate buffer concentration, we propose a two-step model for the protonation of the copper site in agreement with previous crystallographic studies. It is shown that the proton transfer is the rate-limiting step in the reaction at low buffer concentrations, whereas at high buffer concentrations, another step becomes rate-limiting. We suggest that the latter step is a concerted dissociation of His92 from the Cu(I) ion and a 180 degrees rotation of the imidazole ring, which precede the protonation. The first-order rate constant for the dissociation of His92 from the Cu(I) ion is estimated to be 2.4 x 10(4) s(-1). Also, a cooperative effect of the protonation of the remote His61 on the protonation of His92 and the redox properties of the protein was investigated by substituting His61 with asparagine. The mutation causes a modest change in both the pKa value of His92 and the redox potential of the protein.     

Laser-flash photolysis indicates that internal electron transfer is triggered by proton uptake by Alcaligenes xylosoxidans copper-dependent nitrite reductase

Enzyme-catalysed electron transfer reactions are often controlled by protein motions and coupled to chemical change such as proton transfer. We have investigated the nature of this control in the blue copper-dependent nitrite reductase from Alcaligenes xylosoxidans (AxNiR). Inter-Cu electron transfer from the T1Cu site to the T2Cu catalytic site in AxNiR occurs via a proton-coupled electron transfer mechanism. Here we have studied the kinetics of both electron and proton transfer independently using laser-flash photolysis for native AxNiR and its proton-channel mutant N90S. In native AxNiR, both inter-Cu electron transfer and proton transfer exhibit similar rates, and show an unusual dependence on the nitrite concentration. An initial decrease in the observed rates at low nitrite concentrations is followed by an increase in the observed rates at high nitrite concentrations (> 5 mm). In N90S, in which the T1Cu reduction potential is elevated by 60 mV, no inter-Cu electron transfer or proton transfer was observed in the absence of nitrite. Only in the presence of nitrite were both processes detected, with similar [nitrite] dependence, but the nitrite dependence was different compared with native enzyme. The substrate dependence in N90S was similar to that observed in steady-state assays, suggesting that this substitution resulted in proton-coupled electron transfer becoming rate-limiting. A pH perturbation experiment with native AxNiR revealed that protonation triggers inter-Cu electron transfer and generation of NO. Our results show a strong coupling of inter-Cu electron transfer and proton transfer for both native AxNiR and N90S, and provide novel insights into the controlled delivery of electrons and protons to the substrate-utilization T2Cu active site of AxNiR.     

The protonation state of a heme propionate controls electron transfer in cytochrome c oxidase

In cytochrome c oxidase (CcO), exergonic electron transfer reactions from cytochrome c to oxygen drive proton pumping across the membrane. Elucidation of the proton pumping mechanism requires identification of the molecular components involved in the proton transfer reactions and investigation of the coupling between internal electron and proton transfer reactions in CcO. While the proton-input trajectory in CcO is relatively well characterized, the components of the output pathway have not been identified in detail. In this study, we have investigated the pH dependence of electron transfer reactions that are linked to proton translocation in a structural variant of CcO in which Arg481, which interacts with the heme D-ring propionates in a proposed proton output pathway, was replaced with Lys (RK481 CcO). The results show that in RK481 CcO the midpoint potentials of hemes a and a(3) were lowered by approximately 40 and approximately 15 mV, respectively, which stabilizes the reduced state of Cu(A) during reaction of the reduced CcO with O(2). In addition, while the pH dependence of the F --> O rate in wild-type CcO is determined by the protonation state of two protonatable groups with pK(a) values of 6.3 and 9.4, only the high-pK(a) group influences this rate in RK481 CcO. The results indicate that the protonation state of the Arg481 heme a(3) D-ring propionate cluster having a pK(a) of approximately 6.3 modulates the rate of internal electron transfer and may act as an acceptor of pumped protons.     

Electron transfer in reaction centers of Rhodopseudomonas sphaeroides. II. Free energy and kinetic relations between the acceptor states Q(-)A Q(-)B and QAQ(2-)B

Thermodynamic equilibria and electron transfer kinetics involving the quinone acceptor complex in reaction centers from Rhodopseudomonas sphaeroides were investigated. We focussed on reactions involving the two-electron states QA Qn and QAQ~-, described by the scheme DQAQa~-D +X,~~A- , ~~a- ~k~ .~D+ "r~~ AK~'La2- - k~2~ k~lk O~ (2)D+~D The equilibrium partitioning between QA Q n and QAQ 2n- was determined spectroscopically from either the concentration of oxidized cytochrome c or the concentration of semiquinone after successive flashes of light.At pH < 9.5, QAQ2n - is stabilized relative to QAQn, while for pH > 9.5, QAQB is energetically favored.The reduction of QA, to form QAQ~, is not associated with a protonation step (pK< 8). However, the reduction of Q~, to form the final state QAQ~-, is accompanied by an uptake of a proton (pK >/10.7). The preferential interaction of a proton with QAQ2n - provides the driving force for the forward electron transfer.The shift toward the photochemically inactive state QAQa with increasing pH may serve as a feedback mechanism in photosynthetic organisms to limit the rise in intracellular pH. The electron-transfer rate constants were determined from the observed kinetics and the equilibria between the states QAQ2n - and QA Q n. The forward rate constant z-.A~2n~ was approximately proportional to the proton concentration, whereas kta2A~ depended only weakly on pH. The recombination kinetics of D +QAQ2n- was biphasic. The slow rate agreed with the predicted charge recombination via the intermediate state D +QAQff; the fast rate may be due to the recombination from a separate (conformational) state. The results of this work were combined with those of a previous study on reactions involving the one-electron precursor states QAQa and QAQn(Kleinfeld, D., Okamura, M.Y., and Feher, G. (1984) Biochim. Biophys. Acta 766, 126-140). The overall sequence for the protonation of the reaction center in response to successive reductions of the accept or complex involves the uptake of one proton for each electron transferred to QB- This sequential uptake initiates the formation of a proton gradient across the cell membrane.     

Electrochemical modeling of electron and proton transfer to ubiquinone-10 in a self-assembled phospholipid monolayer.

Ubiquinone-10 (UQ) was incorporated at concentrations ranging from 0.5 to 2 mol% in a self-assembled monolayer of dioleoylphosphatidylcholine (DOPC) deposited on a mercury drop electrode, and its electroreduction to ubiquinol (UQH2) was investigated in phosphate and borate buffers over the pH range from 7 to 9.5 by a computerized chronocoulometric technique. The dependence of the applied potential for a constant value of the faradaic charge due to UQ reduction upon the electrolysis time t at constant pH and upon pH at constant t was examined on the basis of a general kinetion approach. This permitted us to conclude that the reduction of UQ to UQH2 in DOPC monolayers takes place via the reversible uptake of one electron with the formation of the semiubiquinone radical anion UQ.-, followed by the rate-determining protonation of this anion with UQH. formation; this neutral radical is more easily reduced than UQ, yielding the ubiquinol UQH2. In spite of the very low concentration of hydrogen ions as compared with that of the acidic component of the buffer, the only effective proton donor is the proton itself; this strongly suggests that the protonation step takes place inside the polar head region of the DOPC monolayer, which is only accessible to protons.     

Proton-transfer kinetics of photoexcited 7-hydroxy-1-naphthalenesulphonic acid in aqueous DMSO solutions.

The monoanion of 7-hydroxy-1-naphthalenesulphonic acid (HNS) undergoes pseudo-first-order dissociation and its conjugate base undergoes second-order protonation in the lowest excited singlet state. The proton transfer kinetics in water containing dimethylsulphoxide (DMSO), up to a mole fraction of about 0.4, have been evaluated as a function of DMSO concentration. At mole fractions above 0.5 of DMSO, proton-transfer does not measurably occur. At mole fractions below 0.5, steady-state and pulsed-source fluorimetries show the rate constant for dissociation to decrease exponentially with increasing mole fraction of DMSO. This is believed to be due to penetration and disruption of the aqueous solvent cage of HNS by DMSO, resulting in impairment of the Grotthus proton-transfer mechanism. The rate of neutralization of the conjugate base by hydrogen ion is found to vary only slightly with solvent composition and depends on the bulk dielectric properties of the solvent.     

Catalytic roles for proton transfer and protonation in ribozymes

Utilization of proton transfer in catalysis, which is well known in the mechanisms of protein enzymes, has been described only relatively recently for RNA enzymes. In this article, we present a current understanding of proton transfer by nucleic acids. Rate enhancement and specificity conferred by general acid-base catalysis are discussed. We also present possibilities for electrostatic catalysis from general acids and bases as well as cationic base pairs. The microenvironments of a large RNA provide the possibility of histidine-like pK(a)s for proton transfer, as well as lysine- and arginine-like pK(a)s for electrostatic catalysis. Discussion on proton transfer focuses on the hepatitis delta virus (HDV) and hairpin ribozymes, with select examples drawn from the protein literature. Discussion on electrostatic catalysis also draws on these two ribozymes, and a postulate for electrostatic catalysis by a cationic base pair in the mechanism of peptidyl transfer in the ribosome is presented. We also provide a perspective on possibilities for phosphoryl transfer mechanisms involving phosphorane intermediates and unusual tautomeric forms of the bases. Lastly, a distinction is made between ground state and "transition state" pK(a)s. We favor a model in which changes in pH lead to changes in the distribution of reactive and nonreactive ionizations of the ribozyme molecules in the ground state, and therefore suggest that "pK(a) changes in the transition state" do not provide an acceptable explanation for observed pH-rate profiles.     

Excited-state dynamics of bacteriorhodopsin.

Near infrared emission of bacteriorhodopsin at neutral pH and at room temperature was characterized by a large Stokes shift. This characteristic was lost in an acidic pH (approximately pH 2) where a remarkable enchancement (more than 10 times) in the fluorescence quantum yield accompanied the red shift in the main absorption band. It is suggested from fluorescence polarization measurements that the emission occurs from the first allowed excited state of the retinylidene chromophore, irrespective of pH. We suggest that the large Stokes shift observed at neutral pH is a result of a charge displacement (e.g., proton translocation) that occurs immediately after excitation, and is prevented by protonation (in the ground state) of an amino-acid residue in the protein.     

Proton transfer in the photoreceptors phytochrome and photoactive yellow protein.

Light-induced activation of the photoreceptors phytochrome and photoactive yellow protein (PYP) is accompanied by protonation changes of the respective chromophores and key residues in the protein moiety. For both systems, proton exchange with the external medium could be observed with pH electrode measurements and with UV-visible absorption spectroscopy using appropriate pH indicator dyes. From these signals, the stoichiometry of proton release and uptake, respectively, was determined by different calibration procedures which will be presented and discussed. Kinetic information on these processes is only available from time-resolved measurements with pH indicator dyes. Vibrational spectroscopy methods such as Fourier transform infrared spectroscopy and resonance Raman scattering provided information on the protonation state of individual functional groups suggesting that internal proton transfer processes are involved as well. Deuterium kinetic isotope effects that occurred in the Pr --> Pfr phototransformation of the bacteriophytochromes Cph1 and Agp1 were consistent with proton transfer reactions as rate-limiting steps. In contrast, the apparent rate constants in the photocycle of PYP exhibited only small kinetic isotope effects that could not be interpreted conclusively. Possible mechanisms of proton transfer in the activation of phytochrome and PYP will be discussed.     

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.     

Sequence-specific DNA binding by the glucocorticoid receptor DNA-binding domain is linked to a salt-dependent histidine protonation

We used isothermal titration calorimetry in the temperature range 21-25 degrees C to investigate the effect of pH on the calorimetric enthalpy (delta H(cal)) for sequence specific DNA-binding of the glucocorticoid receptor DNA-binding domain (GR DBD). Titrations were carried out in solutions containing 100 mM NaCl, 1 mM dithiothreitol, 5% glycerol by volume, and 20 mM Tris, Hepes, Mops, or sodium phosphate buffers at pH 7.5. A strong dependence of delta H(cal) on the buffer ionization enthalpy is observed, demonstrating that the DNA binding of the GR DBD is linked to proton uptake at these conditions. The apparent increase in the pK(a) for an amino acid side chain upon DNA binding is supported by the results of complementary titrations, where delta H(cal) shows a characteristic dependence on the solution pH. delta H(cal) is also a function of the NaCl concentration, with opposite dependencies in Tris and Hepes buffers, respectively, such that a similar delta H(cal) value is approached at 300 mM NaCl. This behavior shows that the DNA-binding induced protonation is inhibited by increased concentrations of NaCl. A comparison with structural data suggests that the protonation involves a histidine (His451) in the GR DBD, because in the complex this residue is located close to a DNA phosphate at an orientation that is consistent with a charged-charged hydrogen bond in the protonated state. NMR spectra show that His451 is not protonated in the unbound protein at pH 7.5. The pH dependence in delta H(cal) can be quantitatively described by a shift of the pK(a) of His451 from approximately 6 in the unbound state to close to 8 when bound to DNA at low salt concentration conditions. A simple model involving a binding competition between a proton and a Na(+) counterion to the GR DBD-DNA complex reproduces the qualitative features of the salt dependence.     

Probing the transition-state structure of dual-specificity protein phosphatases using a physiological substrate mimic

Dual-specificity phosphatases (DSPs) belong to the large family of protein tyrosine phosphatases that contain the active-site motif (H/V)CxxGxxR(S/T), but unlike the tyrosine-specific enzymes, DSPs are able to catalyze the efficient hydrolysis of both phosphotyrosine and phosphoserine/threonine found on signaling proteins, as well as a variety of small-molecule aryl and alkyl phosphates. It is unclear how DSPs accomplish similar reaction rates for phosphoesters, whose reactivity (i.e., pK(a) of the leaving group) can vary by more than 10(8). Here, we utilize the alkyl phosphate m-nitrobenzyl phosphate (mNBP), leaving-group pK(a) = 14.9, as a physiological substrate mimic to probe the mechanism and transition state of the DSP, Vaccinia H1-related (VHR). Detailed pH and kinetic isotope effects of the V/K value for mNBP indicates that VHR reacts with the phosphate dianion of mNBP and that the nonbridge phosphate oxygen atoms are unprotonated in the transition state. (18)O and solvent isotope effects indicate differences in the respective timing of the proton transfer to the leaving group and P-O fission; with the alkyl ester substrate, protonation is ahead of P-O fission, while with the aryl substrate, the two processes are more synchronous. Kinetic analysis of the general-acid mutant D92N with mNBP was consistent with the requirement of Asp-92 in protonating the ester oxygen, either in a step prior to significant P-O bond cleavage or in a concerted but asynchronous mechanism in which protonation is ahead of P-O bond fission. Collectively, the data indicate that VHR and likely all DSPs can match leaving-group potential with the timing of the proton transfer to the ester oxygen, such that diverse aryl and alkyl phosphoesters are turned over with similar catalytic efficiency.     

Buffer catalysis of amino proton exchange in compounds of adenosine, cytidine and their endocyclic N-methylated derivatives

The use of buffer catalysts having a wide range of pK (dissociation) values (4-12) provides the first estimates of two generally useful empirical parameters of amino proton exchange in compounds of adenine and cytosine. These are a nucleobase amino group dissociation constant (pKD) and the 'encounter frequency' for proton transfer (kD), which can be used to predict amino proton exchange rates. Values of amino pKD fall in the range 8.6-9.4 for the unsubstituted nucleobases and their endocyclic N-methylated derivatives. Similar values of kD are obtained for all nucleobases (1 X 10(8) M-1 s-1). These constants were obtained from a statistical fit of second-order catalytic rate constants for amino proton exchange, measured by amino 1H-NMR lineshape at varying field frequencies (100, 300 and 360 MHz). These results confirm the requirement for buffer conjugate base formation and nucleobase protonation, but point to a different mechanism of exchange at low pH; most probably direct amino protonation for adenine, but not for cytosine compounds. Anionic buffer conjugate bases (phosphate and acetate) show a greater catalytic effect than neutral (nitrogen) bases, especially with cytosine compounds. The use of high concentrations of sodium perchlorate to sharpen amino 1H resonances of 1-methyladenosine is examined, with respect to chemical and rotational exchange and NMR line broadening.     

pH-dependence of photo-induced electron transfer in zinc-substituted sperm whale myoglobin

The electron transfer between the excited triplet state of zinc-substituted sperm whale myoglobin and Cu2+ has been studied by following the decay rate of delayed fluorescence. The Cu2+ bound on the surface of the myoglobin molecule are efficient quenchers of the excited electron state of Zn-myoglobin. Two bimolecular rate constants of quenching (KQ) for every pH investigated have been calculated. The pH-dependence of KQ1 indicates that the protonation of one amino acid residue (His-GH1 (119] is important for the process. Our results support the idea of the common nature of the mechanism of quenching by Cu2+ and oxidation of oxymyoglobin by Cu2+.     

Protonation/deprotonation reactions triggered by photoactivation of photoactive yellow protein from Ectothiorhodospira halophila.

Light-dependent pH changes were measured in unbuffered solutions of wild type photoactive yellow protein (PYP) and its H108F and E46Q variants, using two independent techniques: transient absorption changes of added pH indicator dyes and direct readings with a combination pH electrode. Depending on the absolute pH of the sample, a reversible protonation as well as a deprotonation can be observed upon formation of the transient, blue-shifted photocycle intermediate (pB) of this photoreceptor protein. The latter is observed at very alkaline pH, the former at acidic pH values. At neutral pH, however, the formation of the pB state is not paralleled by significant protonation/deprotonation of PYP, as expected for concomitant protonation of the chromophore and deprotonation of Glu-46 during pB formation. We interpret these results as further evidence that a proton is transferred from Glu-46 to the coumaric acid chromophore of PYP, during pB formation. One cannot exclude the possibility, however, that this transfer proceeds through the bulk aqueous phase. Simultaneously, an amino acid side chain(s) (e.g. His-108) changes from a buried to an exposed position. These results, therefore, further support the idea that PYP significantly unfolds in the pB state and resolve the controversy regarding proton transfer during the PYP photocycle.     

Simultaneous replacement of Asp-L210 and Asp-M17 with Asn increases proton uptake by Glu-L212 upon first electron transfer to QB in reaction centers from Rhodobacter sphaeroides.

In the photosynthetic reaction center (RC) from Rhodobacter sphaeroides, the first electron transfer to the secondary quinone acceptor Q(B) is coupled to the protonation of Glu-L212, located approximately 5 A from the center of Q(B). Upon the second electron transfer to Q(B), Glu-L212 is involved in fast proton delivery to the reduced Q(B). Since Asp-L210 and Asp-M17 play an important role in the proton transfer to the Q(B) site [Paddock, M. L., Adelroth, P., Chang, C., Abresch, E. C., Feher, G., and Okamura, M. Y. (2001) Biochemistry 40, 6893-6902], we investigated the effects of replacing one or both Asp residues with Asn on proton uptake by Glu-L212 using FTIR difference spectroscopy. Upon the first electron transfer to Q(B), the amplitude of the proton uptake by Glu-L212 at pH 8 is increased in the single and double mutant RCs, as is evident from the larger intensity (by 35-55%) of the carboxylic acid band at 1727 cm(-1) in the Q(B)(-)/Q(B) difference spectra of mutant RCs, compared to that at 1728 cm(-1) in native RCs. This implies that the extent of ionization of Glu-L212 in the Q(B) ground state is greater in the mutants than in native RCs and that Asp-M17 and Asp-L210 are at least partially ionized near neutral pH in native RCs. In addition, no changes in the protonation state or the environment of these two residues are detected upon Q(B) reduction. The absence of the 1727 cm(-1) signal in all of the RCs lacking Glu-L212, confirms that the positive band at 1728-1727 cm(-1) probes the protonation of Glu-L212 in native and mutant RCs.     

Unraveling the mechanism of proton translocation in the extracellular half‐channel of bacteriorhodopsin

Bacteriorhodopsin, a light activated protein that creates a proton gradient in halobacteria, has long served as a simple model of proton pumps. Within bacteriorhodopsin, several key sites undergo protonation changes during the photocycle, moving protons from the higher pH cytoplasm to the lower pH extracellular side. The mechanism underlying the long‐range proton translocation between the central (the retinal Schiff base SB216, D85, and D212) and exit clusters (E194 and E204) remains elusive. To obtain a dynamic view of the key factors controlling proton translocation, a systematic study using molecular dynamics simulation was performed for eight bacteriorhodopsin models varying in retinal isomer and protonation states of the SB216, D85, D212, and E204. The side‐chain orientation of R82 is determined primarily by the protonation states of the residues in the EC. The side‐chain reorientation of R82 modulates the hydrogen‐bond network and consequently possible pathways of proton transfer. Quantum mechanical intrinsic reaction coordinate calculations of proton‐transfer in the methyl guanidinium‐hydronium‐hydroxide model system show that proton transfer via a guanidinium group requires an initial geometry permitting proton donation and acceptance by the same amine. In all the bacteriorhodopsin models, R82 can form proton wires with both the CC and the EC connected by the same amine. Alternatively, rare proton wires for proton transfer from the CC to the EC without involving R82 were found in an O′ state where the proton on D85 is transferred to D212. Proteins 2016; 84:639–654. © 2016 Wiley Periodicals, Inc.