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

Proton Release Reactions in the Inward H+ Pump NsXeR

Directional ion transport across biological membranes plays a central role in many cellular processes. Elucidating the molecular determinants for vectorial ion transport is key to understanding the functional mechanism of membrane-bound ion pumps. The extensive investigation of the light-driven proton pump bacteriorhodopsin from Halobacterium salinarum(HsBR) enabled a detailed description of outward proton transport. Although the structure of inward-directed proton pumping rhodopsins is very similar to HsBR, little is known about their protonation pathway, and hence, the molecular reasons for the vectoriality of proton translocation remain unclear. Here, we employ a combined experimental and theoretical approach to tracking protonation steps in the light-driven inward proton pump xenorhodopsin from Nanosalina sp. (NsXeR). Time-resolved infrared spectroscopy reveals the transient deprotonation of D220 concomitantly with deprotonation of the retinal Schiff base. Our molecular dynamics simulations support a proton release pathway from the retinal Schiff base via a hydrogen-bonded water wire leading to D220 that could provide a putative gating point for the proton release and with allosteric interactions to the retinal Schiff base. Our findings support the key role of D220 in mediating proton release to the cytoplasmic side and provide evidence that this residue is not the primary proton acceptor of the proton transiently released by the retinal Schiff base.

pH-sensitive vibrational probe reveals a cytoplasmic protonated cluster in bacteriorhodopsin

Infrared spectroscopy has been used in the past to probe the dynamics of internal proton transfer reactions taking place during the functional mechanism of proteins but has remained mostly silent to protonation changes in the aqueous medium. Here, by selectively monitoring vibrational changes of buffer molecules with a temporal resolution of 6 µs, we have traced proton release and uptake events in the light-driven proton-pump bacteriorhodopsin and correlate these to other molecular processes within the protein. We demonstrate that two distinct chemical entities contribute to the temporal evolution and spectral shape of the continuum band, an unusually broad band extending from 2,300 to well below 1,700 cm^-1 The first contribution corresponds to deprotonation of the proton release complex (PRC), a complex in the extracellular domain of bacteriorhodopsin where an excess proton is shared by a cluster of internal water molecules and/or ionic E194/E204 carboxylic groups. We assign the second component of the continuum band to the proton uptake complex, a cluster with an excess proton reminiscent to the PRC but located in the cytoplasmic domain and possibly stabilized by D38. Our findings refine the current interpretation of the continuum band and call for a reevaluation of the last proton transfer steps in bacteriorhodopsin.

Probing biological interfaces by tracing proton passage across them

The properties of water at the surface, especially at an electrically charged one, differ essentially from those in the bulk phase. Here we survey the traits of surface water as inferred from proton pulse experiments with membrane enzymes. In such experiments, protons that are ejected (or captured) by light-triggered enzymes are traced on their way between the membrane surface and the bulk aqueous phase. In several laboratories it has been shown 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 increase in their electric charge, it was suggested that the membrane surface is separated from the bulk aqueous phase by a barrier of electrostatic nature. In terms of ordinary electrostatics, the barrier could be ascribed to dielectric saturation of water at a charged surface. In terms of nonlocal electrostatics, the barrier could result from the dielectric overscreening in the surface water layers. It is discussed how the interfacial potential barrier can affect the reactions at interface, especially those coupled with biological energy conversion and membrane transport.

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 transfer dynamics at membrane/water interface and mechanism of biological energy conversion

Proton transfer between water and the interior of membrane proteins plays a key role in bioenergetics. Here we survey the mechanism of this transfer as inferred from experiments with flash-triggered enzymes capturing or ejecting protons at the membrane surface. These experiments have revealed that proton exchange between the membrane surface and the bulk water phase proceeds at > or =1 msec because of a kinetic barrier for electrically charged species. From the data analysis, the barrier height for protons could be estimated as about 0.12 eV, i.e., high enough to account for the observed retardation in proton exchange. Due to this retardation, the proton activity at the membrane surface might deviate, under steady turnover of proton pumps, from that measured in the adjoining water phase, so that the driving force for ATP synthesis might be higher than inferred from the bulk-to-bulk measurements. This is particularly relevant for alkaliphilic bacteria. The proton diffusion along the membrane surface, on the other hand, is unconstrained and fast, occurring between the neighboring enzymes at less than 1 microsec. The anisotropy of proton dynamics at the membrane surface helps prokaryotes diminish the "futile" escape of pumped protons into the external volume. In some bacteria, the inner membrane is invaginated, so that the "ejected" protons get trapped in the closed space of such intracellular membrane "sacks" which can be round or flat. The chloroplast thylakoids and the mitochondrial cristae have their origin in these intracellular structures.

Site specific labeling of Rhodobacter sphaeroides reaction centers with dye probes for surface pH measurements

Covalently bound pH sensitive dyes are an important tool for characterizing the proteolytic reactions of protein complexes that play key roles in biological energy transduction. Here we demonstrate the feasibility of this method for photosynthetic reaction centers (RCs) for the first time, by the highly selective attachment of two thiol reactive derivatives of fluorescein to the two H subunit cysteines of the photosynthetic RC from Rhodobacter sphaeroides R-26 The pK(a) shifts of the dyes upon binding to the protein and in response to high salt were measured, and interpreted based on the structure of the RC. 2-[(5-fluoresceinyl)aminocarbonyl]ethyl-methanethiosulfonate was attached to Cys H156 and fluorescein-5-maleimide to Cys H234. By following the absorption changes of bound fluorescein (500 nm), and those of the hydrophilic pH indicator 8-hydroxypyrene-1,3,6-tris-sulfonic acid (468 nm), the surface and bulk pH were monitored separately with less than 5% crosstalk. Flash-induced proton uptake and external calibrations by mixing with aliquots of acid were measured in different redox states of the RCs. The results indicate that the charge in the quinone acceptor complex after flash activation (primary quinone acceptor (Q(A))- or secondary quinone acceptor (Q(B))-) has no effect on the surface pH and potential in the vicinity of these two attachment sites, between pH 6.5 and 9. Application of the method to other surface locations is discussed.

Time-resolved FT-IR spectroscopic investigation of the pH-dependent proton transfer reactions in the E194Q mutant of bacteriorhodopsin

The photoreaction of the E194Q mutant of bacteriorhodopsin has been investigated at various pH values by time-resolved step-scan Fourier-transform infrared difference spectroscopy employing the attenuated total reflection technique. The difference spectrum at pH 8.4 is comparable to the N-BR difference spectra of the wild type with the remarkable exception that D85 is deprotonated. Since the retinal configuration is not perturbed by the E194Q mutation, it is concluded that there is no interaction of D85 with retinal during the lifetime of the N state. At pH 6, a consecutive state to the O intermediate is detected in which D212 is transiently protonated. The comparison with wild-type bacteriorhodopsin reveals that protonation of D212 represents an intermediate step during proton transfer from D85 to the proton release group in the final stage of the reaction cycle. The described effects are more pronounced in the E194Q mutant than in the E204Q mutant demonstrating different roles of these two glutamates/glutamic acids at least in the final stages of the catalytic cycle of bacteriorhodopsin.

Time-resolved Fourier transform infrared spectroscopy of the polarizable proton continua and the proton pump mechanism of bacteriorhodopsin

Nanosecond-to-microsecond time-resolved Fourier transform infrared (FTIR) spectroscopy in the 3000-1000-cm(-1) region has been used to examine the polarizable proton continua observed in bacteriorhodopsin (bR) during its photocycle. The difference in the transient FTIR spectra in the time domain between 20 ns and 1 ms shows a broad absorption continuum band in the 2100-1800-cm(-1) region, a bleach continuum band in the 2500-2150-cm(-1) region, and a bleach continuum band above 2700 cm(-1). According to Zundel (G., J. Mol. Struct. 322:33-42), these continua appear in systems capable of forming polarizable hydrogen bonds. The formation of a bleach continuum suggests the presence of a polarizable proton in the ground state that changes during the photocycle. The appearance of a transient absorption continuum suggests a change in the polarizable proton or the appearance of new ones. It is found that each continuum has a rise time of less than 80 ns and a decay time component of approximately 300 micros. In addition, it is found that the absorption continuum in the 2100-1800-cm(-1) region has a slow rise component of 190 ns and a fast decay component of approximately 60 micros. Using these results and those of the recent x-ray structural studies of bR(570) and M(412) (H. Luecke, B. Schobert, H.T. Richter, J.-P. Cartailler, and J. K., Science 286:255-260), together with the already known spectroscopic properties of the different intermediates in the photocycle, the possible origins of the polarizable protons giving rise to these continua during the bR photocycle are proposed. Models of the proton pump are discussed in terms of the changes in these polarizable protons and the hydrogen-bonded chains and in terms of previously known results such as the simultaneous deprotonation of the protonated Schiff base (PSB) and Tyr185 and the disappearance of water molecules in the proton release channel during the proton pump process.

Water and bacteriorhodopsin: structure, dynamics, and function

A wealth of information has been gathered during the past decades that water molecules do play an important role in the structure, dynamics, and function of bacteriorhodopsin (bR) and purple membrane. Light-induced structural alterations in bR as detected by X-ray and neutron diffraction at low and high resolution are discussed in relationship to the mechanism of proton pumping. The analysis of high resolution intermediate structures revealed photon-induced rearrangements of water molecules and hydrogen bonds concomitant with conformational changes in the chromophore and the protein. These observations led to an understanding of key features of the pumping mechanism, especially the vectoriality and the different modes of proton translocation in the proton release and uptake domain of bR. In addition, water molecules influence the function of bR via equilibrium fluctuations, which must occur with adequate amplitude so that energy barriers between conformational states can be overcome.

Bacteriorhodopsin: the functional details of a molecular machine are being resolved

The photon-driven proton translocator bacteriorhodopsin is considered to be the best understood membrane protein so far. It is nowadays regarded as a model system for photosynthesis, ion pumps and seven transmembrane receptors. The profound knowledge came from the applicability of a variety of modern biophysical techniques which have often been further developed with research on bacteriorhodopsin and have delivered major contributions also to other areas. Most prominent examples are electron crystallography, solid-state NMR spectroscopy and time-resolved vibrational spectroscopy. The recently introduced method of crystallising a membrane protein in the lipidic cubic phase led to high-resolution structures of ground state bacteriorhodopsin and some of the photocycle intermediates. This achievement in combination with spectroscopic results will strongly advance our understanding of the functional mechanism of bacteriorhodopsin on the atomic level. We present here the current knowledge on specific aspects of the structural and functional dynamics of the photoreaction of bacteriorhodopsin with a focus on techniques established in our institute.

Buffer effects on electric signals of light-excited bacteriorhodopsin

Buffers change the electric signals of light-excited bacteriorhodopsin molecules in purple membrane if their concentration and the pH of the low-salt solution are properly selected. "Positive" buffers produce a positive component, and "negative" buffers a negative component in addition to the signals due to proton pumping. Measurement of the buffer effects in the presence of glycyl-glycine or bis-tris propane revealed an increase of approximately 2 and a change of sign and a decrease to approximately -0.5 in the translocated charge in these cases, respectively. These factors do not depend on temperature. The Arrhenius parameters established from the evaluation of the kinetics indicate activation enthalpies of 35-40 kJ/mol and negative activation entropies for the additional signals. These values agree with those found by surface-bound pH-sensitive probes in the search of the timing of proton release and uptake. The electric signals were also measured in the case of D(2)O solutions with similar results, except for the increased lifetimes. We offer a unified explanation for the data obtained with surface-bound probes and electric signals based on the clusters at extracellular and cytoplasmic sites of bacteriorhodopsin participating in proton release and uptake.

Proton transfer reactions across bacteriorhodopsin and along the membrane

Bacteriorhodopsin is probably the best understood proton pump so far and is considered to be a model system for proton translocating membrane proteins. The basis of a molecular description of proton translocation is set by having the luxury of six highly resolved structural models at hand. Details of the mechanism and reaction dynamics were elucidated by a whole variety of biophysical techniques. The current molecular picture of catalysis by BR will be presented with examples from time-resolved spectroscopy. FT-IR spectroscopy monitors single proton transfer events within bacteriorhodopsin and judiciously positioned pH indicators detect proton migration at the membrane surface. Emerging properties are briefly outlined that underlie the efficient proton transfer across and along biological membranes.

Opening the Schiff base moiety of bacteriorhodopsin by mutation of the four extracellular Glu side chains

The quadruple bacteriorhodopsin (BR) mutant E9Q+E74Q+E194Q+E204Q shows a lambda(max) of about 500 nm in water at neutral pH and a great influence of pH and salts on the visible absorption spectrum. Accessibility to the Schiff base is strongly increased, as detected by the rapid bleaching effect of hydroxylamine in the dark as well as in light. Both the proton release kinetics and the photocycle are altered, as indicated by a delayed proton release after proton uptake and changed M kinetics. Moreover, affinity of the color-controlling cation(s) is found to be decreased. We suggest that the four Glu side chains are essential elements of the extracellular structure of BR.

Bacteriorhodopsin

Bacteriorhodopsin is a seven-transmembrane helical protein that contains all-trans retinal. In this light-driven pump, a reaction cycle initiated by photoisomerization to 13-cis causes translocation of a proton across the membrane. Local changes in the geometry of the protonated Schiff base and the proton acceptor Asp85, and the proton conductivities of the half channels that lead from this active site to the two membrane surfaces, interact so as to allow timely proton transfers that result in proton release on the extracellular side and proton uptake on the cytoplasmic one. The details of the steps in this photocycle, and the underlying principles that ensure unidirectionality of the movement of a proton across the protein, provide strong clues to how ion pumps function.

Bacteriorhodopsin's intramolecular proton-release pathway consists of a hydrogen-bonded network

In its proton-pumping photocycle, bacteriorhodopsin releases a proton to the extracellular surface at pH 7 in the transition from intermediate L to intermediate M. The proton-release group, named XH, was assigned in low-temperature FT-IR studies to a single residue, E204 [Brown, L. S., Sasaki, J., Kandori, H., Maeda, A., Needleman, R. , and Lanyi, J. K. (1995) J. Biol. Chem. 270, 27122-27126]. The time-resolved room-temperature step-scan FT-IR photocycle studies on wild-type and E204Q-, and E204D-mutated bacteriorhodopsin, which we present here, show in contrast that the FT-IR data give no evidence for deprotonation of E204 in the L-to-M transition. Therefore, it is unlikely that E204 represents XH. On the other hand, IR continuum absorbance changes indicate intramolecular proton transfer via an H-bonded network to the surface of the protein. It appears that this H-bonded network is spanned between the Schiff base and the protein surface. The network consists at least partly of internally bound water molecules and is stabilized by E204 and R82. Other not yet identified groups may also contribute. At pH 5, the intramolecular proton transfer to the surface of the protein seems not to be disturbed. The proton seems to be buffered at the surface and later in the photocycle released into the bulk during BR recovery. Intramolecular proton transfer via a complex H-bonded network is proposed to be a general feature of proton transfer in proteins.

Dehydration of biological membranes by cooling: an investigation on the purple membrane

The lamellar spacing dl of purple membrane (PM) multilayer systems was investigated with neutron diffraction as a function of temperature and of the level of hydration. The observed large T-dependent variations of dl indicate that PM is partially dehydrated when cooled below a "hydration water freezing point". This phenomenon is reversible, but a hysteresis is observed when PM is rehydrated upon reheating. The hydration water remaining bound to the membrane below about 240 K is non-freezing. Its amount was found to be hnf=0.24(+/-0.02) g 2H2O/g BR for all samples equilibrated at room temperature in the presence of 2H2O vapour at >/=84% r.h. It is evident, that the dehydration/rehydration behaviour of PM is strongly correlated with the temperature-dependent behaviour of the dynamical structure factor. Above the well-known "dynamical transition" announcing the onset of localized diffusive molecular motions between 190 K and 230 K, a second dynamical transition is caused by the temperature-induced rehydration of the PM starting near 255 K. This is also correlated with the deviation from a pure Arrhenius law of the rate-limiting process in the photocycle, known to occur upon cooling beyond the ice point into the same temperature region. Our results suggest that the phenomenon of dehydration and rehydration induced by cooling and reheating, respectively, is a general property of biological membranes.

Mechanism of proton entry into the cytoplasmic section of the proton-conducting channel of bacteriorhodopsin

Bacteriorhodopsin is the light-driven proton-pumping protein of Halobacterium salinarum that extracts protons from the well-buffered cytoplasmic space within the time limits set by the photocycle turnover. The specific mechanism of the proton uptake by the cytoplasmic surface of the protein was investigated in this study by the laser-induced proton pulse technique. The purple membrane preparations were labeled by fluorescein at two residues (36 or 38) of the cytoplasmic surface of the protein, sites that are close to the orifice of the proton-conducting channel. The membranes were pulsed by protons discharged from photoexcited pyranine [Nachliel, E., Gutman, M., Kiryati, S., and Dencher, N.A. (1996) Proc. Nat Acad. Sci. U.S.A. 93, 10747-10752). The reaction of the discharged protons with the pyranine anion and the fluorescein was measured with sub-microsecond resolution. The experimental signals were reconstructed through numeric integration of differential rate equations which quantitated the rates of all proton transfer reactions between all reactants present in the system. The interaction of protons with the orifice of the cytoplasmic channel is enhanced by the exposed carboxylates of the protein. A cluster of three carboxylates acts as a strong proton attractor site while one carboxylate, identified as D36, acts as a mediator that delivers the proton to the channel. The combination of these reactions render the surface of the protein with properties of a proton-collecting antenna. The size of the collecting area is less than that of the protein's surface.

Mutation of a surface residue, lysine-129, reverses the order of proton release and uptake in bacteriorhodopsin; guanidine hydrochloride restores it

K129 is a residue located in the extracellular loop connecting transmembrane helices D and E of bacteriorhodopsin. Replacement of K129 with a histidine alters the pKa's of two key residues in the proton transport pathway, D85, and the proton release group (probably E204); the resulting pigment has properties that differ markedly from the wild type. 1) In the unphotolyzed state of the K129H mutant, the pKa of D85 is 5.1 +/- 0.1 in 150 mM KCl (compared to approximately 2.6 in the wild-type bacteriorhodopsin), whereas the unphotolyzed-state pKa of E204 decreases to 8.1 +/- 0.1 (from approximately 9.5 in the wild-type pigment). 2) The pKa of E204 in the M state is 7.0 +/- 0.1 in K129H, compared to approximately 5.8 in the wild-type pigment. 3) As a result of the change in the pKa of E204 in M, the order of light-induced proton release and uptake exhibits a dependence on pH in K129H differing from that of the wild type: at neutral pH and moderate salt concentrations (150 mM KCl), light-induced proton uptake precedes proton release, whereas it follows proton release at higher pH. This pumping behavior is similar to that seen in a related bacterial rhodopsin, archaerhodopsin-1, which has a histidine in the position analogous to K129. 4) At alkaline pH, a substantial fraction of all-trans K129H pigment (approximately 30%) undergoes a conversion into a shorter wavelength species, P480, with pKa approximately 8.1, close to the pKa of E204. 5) Guanidine hydrochloride lowers the pKa's of D85 and E204 in the ground state and the pKa of E204 in the M intermediate, and restores the normal order of proton release before uptake at neutral pH. 6) In the K129H mutant the coupling between D85 and E204 is weaker than in wild-type bacteriorhodopsin. In the unphotolyzed pigment, the change in the pKa's of either residue when the other changes its protonation state is only 1.5 units compared to 4.9 units in wild-type bacteriorhodopsin. In the M state of photolyzed K129H pigment, the corresponding change is 1 unit, compared to 3.7 units in the wild-type pigment. We suggest that K129 may be involved in stabilizing the hydrogen bonding network that couples E204 and D85. Substitution of K129 with a histidine residue causes structural changes that alter this coupling and affect the pKa's of E204 and D85.

Protonation dynamics of the extracellular and cytoplasmic surface of bacteriorhodopsin in the purple membrane

The dynamics of proton binding to the extracellular and the cytoplasmic surfaces of the purple membrane were measured by laser-induced proton pulses. Purple membranes, selectively labeled by fluorescein at Lys-129 of bacteriorhodopsin, were pulsed by protons released in the aqueous bulk from excited pyranine (8-hydroxy-1,3,6-pyrenetrisulfonate) and the reaction of protons with the indicators was measured. Kinetic analysis of the data imply that the two faces of the membrane differ in their buffer capacities and in their rates of interaction with bulk protons. The extracellular surface of the purple membrane contains one anionic proton binding site per protein molecule with pK = 5.1. This site is within a Coulomb cage radius (approximately 15 A) from Lys-129. The cytoplasmic surface of the purple membrane bears 4-5 protonable moieties (pK = 5.1) that, due to close proximity, function as a common proton binding site. The reaction of the proton with this cluster is at a very fast rate (3.10(10) M-1.s-1). The proximity between the elements is sufficiently high that even in 100 mM NaCl they still function as a cluster. Extraction of the chromophore retinal from the protein has a marked effect on the carboxylates of the cytoplasmic surface, and two to three of them assume positions that almost bar their reaction with bulk protons. The protonation dynamics determined at the surface of the purple membrane is of relevance both for the vectorial proton transport mechanism of bacteriorhodopsin and for energy coupling, not only in halobacteria, but also in complex chemiosmotic systems such as mitochondrial and thylakoid membranes.

Quantitative evaluation of the dynamics of proton transfer from photoactivated bacteriorhodopsin to the bulk

It has been reported by many research groups that protons released during the photocycle of bacteriorhodopsin are detected by surface bound indicators much faster than by indicators in the bulk. In this study we used numerical simulation of chemical reaction's dynamics for analyzing the delayed appearance of protons in the bulk. The results indicate that the low pK surface groups of the membrane, which form an undilutable concentrated matrix of proton binding sites, retain the protons in this space according to the mass action law. The main sites for proton accumulation are the cluster of carboxylates on the cytoplasmic side of the membrane. The protonation of an indicator in the bulk does not proceed by its reaction with free proton, but rather through self-diffusion of the indicator to the membrane and abstraction of proton from the protonated surface group. The detailed mechanisms which correspond with these reactions are reported.

D38 is an essential part of the proton translocation pathway in bacteriorhodopsin

At present, almost no knowledge exists about the functional relevance of the amino acid residues at the cytoplasmic (CP) surface of the light-driven proton pump bacteriorhodopsin (BR) although a prerequisite for efficient vectorial proton translocation is the efficient capture of protons from the alkaline cytoplasm of the cell. To identify residues involved in the proton transfer reaction steps in the CP part of BR, the aspartic and glutamic amino acids D36, D38, D102, D104, and E161 were replaced by cysteine and arginine (i.e., a negatively charged residue by a neutral or positive one at the pH of investigation). The effect of these replacements on the photo- and transport cycle was examined by time-resolved visible and infrared spectroscopy, biochemical modification studies, and activity assays in intact cells. Of the five CP amino acids studied, only the replacement of D38 resulted in severe alterations of the reaction steps in BR during the second half of the photocycle. Our data show that D38, which seemed to be a freely accessible CP surface residue lacking functional importance, is an essential part of the CP proton uptake pathway connecting the membrane surface with the Schiff base of BR, probably as the first amino acid residue at the CP entrance. D38 influences the late steps in the functional cycle, such as the occurrence of the intermediates N and O, the modulation of the hydrogen-network, the conformational changes in the protein moiety, and the deprotonation/reprotonation of D96. Opposed to this function, the surface-exposed amino acids D36, D102, D104, and E161 seem to efficiently collect protons from the aqueous bulk phase and funnel them to the entrance of the CP proton pathway.

Experimental evidence for hydrogen-bonded network proton transfer in bacteriorhodopsin shown by Fourier-transform infrared spectroscopy using azide as catalyst

Experimental evidence for proton transfer via a hydrogen-bonded network in a membrane protein is presented. Bacteriorhodopsin's proton transfer mechanism on the proton uptake pathway between Asp-96 and the Schiff base in the M-to-N transition was determined. The slowdown of this transfer by removal of the proton donor in the Asp-96-->Asn mutant can be accelerated again by addition of small weak acid anions such as azide. Fourier-transform infrared experiments show in the Asp-96-->Asn mutant a transient protonation of azide bound to the protein in the M-to-N transition and, due to the addition of azide, restoration of the IR continuum band changes as seen in wild-type bR during proton pumping. The continuum band changes indicate fast proton transfer on the uptake pathway in a hydrogen-bonded network for wild-type bR and the Asp-96-->Asn mutant with azide. Since azide is able to catalyze proton transfer steps also in several kinetically defective bR mutants and in other membrane proteins, our finding might point to a general element of proton transfer mechanisms in proteins.

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.

Reorientations in the bacteriorhodopsin photocycle

Reversible photoinduced reorientations of bacteriorhodopsin have been detected in suspensions of the purple membrane of Halobacterium salinarium. The anisotropy in bacteriorhodopsin during the nanosecond through millisecond stages of the photocycle was measured by time-resolved linear dichroism and transient absorption measurements. From these measurements the anisotropies of the K, L, M, and O intermediates were determined and related to the chromophore orientation with respect to the initially selected orientation. The anisotropies of the K and L states are 0.38 +/- 0.01 and 0.35 +/- 0.01, respectively. Further anisotropy decay after formation of the M intermediate in about 0.5 ms is evidence of orientational motion at this stage in the photocycle. A constant anisotropy with a value of 0.39 +/- 0.02 in the O intermediate demonstrates a recovery of the initial protein orientation with the formation of the O state. These results demonstrate that reorientations in BR are photoinduced and reversible. Similar measurements for L and M were carried out for purple membrane in polyacrylamide gels, where the anisotropies in the L and M states are 0.38 +/- 0.014 and 0.36 +/- 0.01, respectively. These results show that reorientations also occur in BR immobilized in gels. Anisotropy decay in the M state after formation of the M intermediate was not detected in the gels, in contrast to the M intermediate in suspensions. Orientational changes are observed for BR in purple membrane suspensions in the K state, during the K-->L step, in the M state possibly related to an M1-->M2 transition, and in the O state, where an almost complete return to the original orientation occurs.(ABSTRACT TRUNCATED AT 250 WORDS)

Proton migration along the membrane surface and retarded surface to bulk transfer

Since the proposal of the chemiosmotic theory there has been a continuing debate about how protons that have been pumped across membranes reach another membrane protein that utilizes the established pH gradient. Evidence has been gathered in favour of a 'delocalized' theory, in which the pumped protons equilibrate with the aqueous bulk phase before being consumed, and a 'localized' one, in which protons move exclusively along the membrane surface. We report here that after proton release by an integral membrane protein, long-range proton transfer along the membrane surface is faster than proton exchange with the bulk water phase. The rate of lateral proton diffusion can be calculated by considering the buffer capacity of the membrane surface. Our results suggest that protons can efficiently diffuse along the membrane surface between a source and a sink (for example H(+)-ATP synthase) without dissipation losses into the aqueous bulk.

Proton lateral conduction along a lipid monolayer spread on a physiological subphase

A localized lateral proton pathway is present along the phospholipid polar heads and bound water molecules when the lipids are spread in monolayers at the air/water interface. Conduction can be detected on concentrated buffers as found under physiological conditions if the lateral proton gradient is large enough. The localized movement supports the occurrence of microlocalized proton circuits along a membrane and of lateral proton gradients.

pH dependence of the absorption spectra and photochemical transformations of the archaerhodopsins

Two strains of archaebacteria have been found to contain light-driven proton pumping pigments analogous to bacteriorhodopsin (bR) in Halobacterium salinarium. These proteins are called archaerhodopsin-1 (aR-1) and archaerhodopsin-2 (aR-2). Their high degree of sequence identity with bR within the putative proton channel enables us to draw some conclusions about the roles of regions where differences in amino acids exist, and in particular the surface residues, on the structure and function of retinal-based proton pumps. We have characterized the spectral and photochemical properties of these two proteins and compared them to the corresponding properties of bR. While there are some differences in absorbance maxima and kinetics of the photocycle, most of the properties of aR-1 and aR-2 are similar to those of bR. The most striking differences of these proteins with bR are the lack of an alkaline-induced red-shifted absorption species and a dramatic (apparent) decrease in the light-induced transient proton release. In membrane sheet suspensions of aR-1 at 0.15 M KCl, the order of proton release and uptake appears opposite that of bR, in which proton release precedes uptake. The nature of this behavior appears to be due to differences in the amino acid sequence at the surfaces of the proteins. In particular, the residue corresponding to the lysine at position 129 of the extracellular loop region of bR is a histidine in aR-1 and could regulate the efficient release of protons into solution in bR.

Proton translocation mechanism and energetics in the light-driven pump bacteriorhodopsin

In spite of many still unsolved problems, the mechanism and energetics of the light-driven proton transport are now basically understood. Energy captured during photoexcitation, and retained in the form of bond rotations and strains of the retinal, is transformed into directed changes in the pKa values of vectorially arranged proton transfer groups. The framework for the spatial and temporal organization of these changes is provided by the protein near the retinal Schiff base. The transport is completed by proton transfer among three essential groups in three domains lying roughly parallel with the membrane plane (Fig. 1): (a) the anionic D85 that is included in a complex of residues on the extracellular side containing also R82, D212, Y57 and bound water; (b) the protonated Schiff base; and (c) the protonated D96 that is included in a complex of residues on the cytoplasmic side containing also R227, T46, S226, and bound water. Other neighboring polar groups and water bound elsewhere which play a role in the transport do so either by further influencing the pKa values of the three protonable groups, or by providing passive pathways for proton transfer. The Schiff base proton, destabilized after photoexcitation, is transferred to the low pKa group D85 located on the extracellular side. The access of the deprotonated Schiff base then changes to the cytoplasmic side (the 'reprotonation switch') and its proton affinity increases. Finally, the proton of the high pKa group D96, with access to the cytoplasmic side, is destabilized by a protein conformational change through rearrangement of R227, T46, S226 and bound water, and becomes transferred to the Schiff base. As shown schematically in Fig. 3, these internal events are coupled to proton release and uptake at the two aqueous surfaces. The charge of the extracellular hydrogen-bonded complex is redistributed upon protonation of D85, and if the pH is above the pKa of the complex a proton is released to the bulk. After reprotonation of the Schiff base the pKa of the cytoplasmic hydrogen-bonded complex is raised well above the pH, and D96 regains a proton from the bulk. If the pH is lower than the pKa of the extracellular complex the proton release is delayed until the end of the photocycle. In either sequence there is net transfer of a proton from the cytoplasmic to the extracellular phase. The transfer of excess free energy from the chromophore to the protein, and finally to the transported proton, is described by a characteristic thermodynamic cycle.(ABSTRACT TRUNCATED AT 400 WORDS)

Relationship of proton uptake on the cytoplasmic surface and reisomerization of the retinal in the bacteriorhodopsin photocycle: an attempt to understand the complex kinetics of the pH changes and the N and O intermediates

In the bacteriorhodopsin photocycle the recovery of the initial BR state from the M intermediate occurs via the N and O intermediates. The molecular events in this process include reprotonation of the Schiff base and the subsequent uptake of a proton from the cytoplasmic side, as well as reisomerization of the retinal from 13-cis to all-trans. We have studied the kinetics of the intermediates and the proton uptake. At moderately low pH little of the N state accumulates, and the O state dominates in the reactions that lead from M to BR. The proton uptake lags behind the formation of O, suggesting the sequence N(0)<==>O(0) + H+ (from the bulk)-->O(+1)-->BR+H+ (to the bulk), where the superscripts indicate the net protonation state of the protein relative to BR. Together with a parallel study of ours at moderately high pH, these results suggest that the sequence of proton uptake and retinal reisomerization depends on pH: at low pH the isomerization occurs first and O accumulates, but at high pH the isomerization is delayed and therefore N accumulates. Although this model contains too many rate constants for rigorous testing, we find that it will generate most of the characteristic pH-dependent kinetic features of the photocycle with few assumptions other than pH dependency for protonation at the proton release and uptake steps.

Evidence in favor of the existence of a kinetic barrier for proton transfer from a surface of bilayer phospholipid membrane to bulk water

When the hydrogen-ion flux is induced by nigericin across the planar bilayer lipid membrane (BLM) with bulk pH values being equal at the opposite sides of the BLM, formation of a difference in boundary potentials (delta phi b) on the membrane is observed by the method of inner membrane field compensation. pH gradients are titrated routinely by the addition of sodium acetate at one side of the membrane. The increase in buffer concentration (citrate, phosphate, Mes) leads to a decrease in delta phi b. delta phi b forms in the presence of phosphatidylserine in the membrane-forming solution only. It is concluded that the steady-state difference of the hydrogen ion binding to the opposite surfaces of the membrane (HIBD) is created under the conditions of equal pH values near surfaces of the BLM. The model of the processes implies that nigericin transfers proton predominantly from interface to interface while acetate transfers the proton from bulk phase to bulk phase. In the other series of experiments the monensin-mediated formation of the HIBD leads to the formation of an potassium-ion gradient in the presence of nigericin. Thus, a possibility of performing a work due to the formation of HIBD is demonstrated. Owing to these properties the hydrogen-ion binding difference can be interpreted in a first approximation as a difference of surface hydrogen-ion concentration at the opposite sides of the membrane, arising due to the existence of a kinetic barrier for the proton transfer at the membrane interfaces. These findings can be significant for the mechanism of energy transduction in membrane phosphorylation in mitochondria and chloroplasts.

Bacteriorhodopsin expressed in Schizosaccharomyces pombe pumps protons through the plasma membrane

Bacterioopsin (bO) from Halobacterium salinarium ("Halobacterium halobium") has been functionally expressed in a heterologous system, the fission yeast Schizosaccharomyces pombe. Regeneration of bO to bacteriorhodopsin (bR) in S. pombe has been achieved in vivo by addition of the chromophore retinal to the culture medium, as shown for a retinal-negative mutant of H. salinarium (JW5). Western blot analysis revealed that bR is more stable than bO against proteolysis in fission yeast and also in JW5. The light-driven proton pump is expressed in the eukaryotic organism and incorporated into the plasma membrane. Illumination of intact yeast cells leads to acidification of the external medium due to the translocation of H+ from inside to outside of the cell, indicating the same orientation of bR in the yeast plasma membrane as in H. salinarium. The kinetics of proton release into the water phase was observed with the optical pH indicator pyranine. Time-resolved absorbance changes of isolated plasma membrane measured by flash spectroscopy showed rise and decay of the M intermediate during the photocycle similar to those in the homologous system. Photocurrents and photovoltages were recorded with yeast plasma membrane attached to a planar lipid membrane and to a polytetrafluoroethylene (Teflon) film, respectively. Stationary currents measured in the presence of a protonophore showed continuous pumping activity of bR. The action spectrum of the photocurrent and the kinetics of the photovoltage were analyzed and compared with signals obtained from purple membranes. From all these different investigations we conclude that the integral membrane protein bR is correctly folded in vivo into the cytoplasmic membrane of the fission yeast S. pombe.

Proton transfer from Asp-96 to the bacteriorhodopsin Schiff base is caused by a decrease of the pKa of Asp-96 which follows a protein backbone conformational change

In the bacteriorhodopsin photocycle the transported proton crosses the major part of the hydrophobic barrier during the M to N reaction; in this step the Schiff base near the middle of the protein is reprotonated from D96 located near the cytoplasmic surface. In the recombinant D212N protein at pH > 6, the Schiff base remains protonated throughout the photocycle [Needleman, Chang, Ni, Váró, Fornés, White, & Lanyi (1991) J. Biol. Chem. 266, 11478-11484]. Time-resolved difference spectra in the visible and infrared are described by the kinetic scheme BR-->K<==>L<==>N (-->N')-->BR. As evidenced by the large negative 1742-cm-1 band of the COOH group of the carboxylic acid, deprotonation of D96 in the N state takes place in spite of the absence of the unprotonated Schiff base acceptor group of the M intermediate. Instead of internal proton transfer to the Schiff base, the proton is released to the bulk, and can be detected with the indicator dye pyranine during the accumulation of N'. The D212N/D96N protein has a similar photocycle, but no proton is released. As in wild-type, deprotonation of D96 in the N state is accompanied by a protein backbone conformational change indicated by characteristic amide I and II bands. In D212N the residue D96 can thus deprotonate independent of the Schiff base, but perhaps dependent on the detected protein conformational change. This could occur through increased charge interaction between D96 and R227 and/or increased hydration near D96. We suggest that the proton transfer from D96 to the Schiff base in the wild-type photocycle is driven also by such a decrease in the pKa of D96.

Surface-bound optical probes monitor protein translocation and surface potential changes during the bacteriorhodopsin photocycle

Light-induced H+ release and reuptake as well as surface potential changes inherent in the bacterio-rhodopsin reaction cycle were measured between 10 degrees C and 50 degrees C. Signals of optical pH indicators covalently bound to Lys-129 at the extracellular surface of bacteriorhodopsin were compared with absorbance changes of probes residing in the aqueous bulk phase. Only surface-bound indicators monitor the kinetics of H+ ejection from bacteriorhodopsin and allow the correlation of the photocycle with the pumping cycle. During the L550----M412 transition the H+ appears at the extracellular surface of bacteriorhodopsin. Surface potential changes detected by bound fluorescein or by the potentiometric probe 4-[2-(di-n-butylamino)-6-naphthyl]vinyl-1-(3-sulfopropyl)pyridinium betaine (di-4-ANEPPS) occur in milliseconds concomitantly with the formation and decay of the N intermediate. pH indicators residing in the aqueous bulk phase reflect the transfer of H+ from the membrane surface into the bulk but do not probe the early events of H+ pumping. The observed retardation of H+ at the membrane surface for several hundred microseconds is of relevance for energy conversion of biological membranes powered by electrochemical H+ gradients.

Asp85 is the only internal aspartic acid that gets protonated in the M intermediate and the purple-to-blue transition of bacteriorhodopsin. A solid-state 13C CP-MAS NMR investigation

High-resolution solid-state 13C NMR spectra of the ground state and M intermediate of the bacteriorhodopsin mutant D96N with the isotope label at [4-13C]Asp and [11-13C]Trp were recorded. The NMR spectra show that Asp85 is protonated in the M intermediate. The environment of Asp85 is quite hydrophobic. On the other hand, Asp212 remains deprotonated and a slight shift to lower field indicates a more hydrophilic environment. Asp85 also protonates in the purple-to-blue transition of bacteriorhodopsin in the deionized membrane, where it experiences a similar environment to M. The shift of Trp resonances in M reflect a conformational change of the protein in forming the M intermediate.

A unifying concept for ion translocation by retinal proteins

First, halorhodopsin is capable of pumping protons after illumination with green and blue light in the same direction as chloride. Second, mutated bacteriorhodopsin where the proton acceptor Asp85 and the proton donor Asp96 are replaced by Asn showed proton pump activity after illumination with blue light in the same direction as wildtype after green light illumination. These results can be explained by and are discussed in light of our new hypothesis: structural changes in either molecule lead to a change in ion affinity and accessibility for determining the vectoriality of the transport through the two proteins.

Proton transfer and energy coupling in the bacteriorhodopsin photocycle

A description of the rate constants and the energetics of the elementary reaction steps of the photocycle of bacteriorhodopsin has been helpful in understanding the mechanism of proton transport in this light-driven pump. The evidence suggests a single unbranched reaction sequence, BR-hv----K in equilibrium with L in equilibrium with M1----M2 in equilibrium with N in equilibrium with O----BR, where coupling to the proton-motive force is at the energetically and mechanistically important M1----M2 step. The consequences of site-specific mutations expressed homologously in Halobacterium halobium have revealed characteristics of the Schiff base deprotonation in the L----M1 reaction, the reorientation of the Schiff base from the extracellular to the cytoplasmic side in the M1----M2 reaction, and the reprotonation of the Schiff base in the M2----N reaction.