The retinylidene Schiff base counterion in bacteriorhodopsin

Previous studies of bacteriorhodopsin have indicated interactions between Asp-85, Asp-212, Arg-82, and the retinylidene Schiff base. The counterion environment of the Schiff base has now been further investigated by using single and double mutants of the above amino acids. Chromophore regeneration from bacterioopsin proceeds to a normal extent in the presence of a single aspartate or glutamate residue at position 85 or 212, whereas replacement of both charged amino acids in the mutant Asp-85----Asn/Asp-212----Asn abolishes the binding of retinal. This indicates that a carboxylate group at either residue 85 or 212 is required as counterion for formation and for stabilization of the protonated Schiff base. Measurements of the pKa of the Schiff base reveal reductions of greater than 3.5 units for neutral single mutants of Asp-85 but only decreases of less than 1.2 units for corresponding substitutions of Asp-212, relative to the wild type. Substitutions of Asp-85 show large red shifts in the absorption spectrum that are partially reversible upon addition of anions, whereas mutants of Asp-212 display minor red shifts or blue shifts. We conclude, therefore, that Asp-85 is the retinylidene Schiff base counterion in wild-type bacteriorhodopsin. In the mutant Asp-85----Asn/Asp-212----Asn formation of a protonated Schiff base chromophore is restored in the presence of salts. The spectral properties of the double mutant are similar to those of the acid-purple form of bacteriorhodopsin. Upon addition of salts the folded structure of wild-type and mutant proteins can be stabilized at low pH in lipid/detergent micelles. The data indicate that exogenous anions serve as surrogate counterions to the protonated Schiff base, when the intrinsic counterions have been neutralized by mutation or by protonation.     

Effects of tryptophan mutation on the deprotonation and reprotonation kinetics of the Schiff base during the photocycle of bacteriorhodopsin.

The rates of deprotonation and reprotonation of the protonated Schiff base (PSB) are determined during the photocycle of nine bacteriorhodopsin mutants in which Trp-10, 12, 80, 86, 137, 138, 182 and 189 are individually substituted by either phenylalanine or cysteine. Of all the mutants, the replacement of Trp-86, Trp-182, and Trp-189 by phenylalanine and Trp-137 by cysteine is found to significantly alter the rate of the deprotonation, but not that of the reprotonation process. As compared with ebR, the Trp-86 mutation dramatically increases the rate of deprotonation of the PSB while the Trp-182 mutation greatly decreases this rate. Temperature dependence studies on the rate constants of the deprotonation demonstrate that the different energetic and entropic effects of the mutation are responsible for the observed different kinetic behavior of the Trp-86 and Trp-182 mutants as compared with that of ebR. In the case of Trp-86 mutant, a large decrease in both energy and entropy of activation suggests that the mutation of this tryptophan residue opens up the protein structure as a result of eliminating the hydrogen-bonding group on its side chain by a phenylalanine substitution. A correlation is observed between the proton pumping yield and the relative amplitudes of the slow deprotonation component but not with rate constants of the rise or decay process at constant pH. These results are best discussed in terms of the heterogeneity model (with parallel cycle) rather than back reaction model.     

Effect of iodination on the pK of Schiff base deprotonation and M412 production in purple membrane

Previously, kinetic resonance Raman measurements as a function of pH have been used to demonstrate that, microseconds after light absorption, the pK of Schiff base deprotonation during the bacteriorhodopsin photocycle is 10.2 ± 0.3, whereas before the light event, the pK is > 12 (2). In this investigation, we have iodinated purple membrane suspensions and have found that the pK of Schiff base deprotonation in the photocycle has been lowered to between 7 and 8 for iodinated bacteriorhodopsin. These results, together with our previous data on the pK of Schiff base deprotonation, suggest that the amino acid tyrosine could be a critical component in the deprotonation mechanism.     

Kinetic and spectroscopic evidence for an irreversible step between deprotonation and reprotonation of the Schiff base in the bacteriorhodopsin photocycle.

The photocycles of wild-type bacteriorhodopsin and its D96N form were investigated with a gated multichannel analyzer. Reconstruction of the spectra of the photointermediates from the measured time-resolved difference spectra allowed evaluation of the kinetics; the data at pH 7 in the presence of 100 mM NaCl were best fitted by the scheme K in eqiulibrium L in equilibrium M1----M2 in equilibrium N in equilibrium O----BR plus N----BR [Váró, G., & Lanyi, J. K. (1990) Biochemistry 29, 2241-2250]. The proposed two M states and the M1----M2 reaction were necessitated by anomalies in the kinetics of the decay of K and L. Additional support was provided by a 4-nm blue-shift in the maximum of M in Triton X-100 solubilized bacteriorhodopsin during the photocycle; the kinetics of the shift were consistent with the time course of the proposed M1----M2 transition. In the D96N mutant, the M state is stabilized, and the resulting equilibrium mixture for the intermediates could be evaluated with greater precision. The concentration ratio of L to M at the equilibrium was estimated to be no higher than 0.01. This requires the ratio of forward/reverse rates for the M1 to M2 conversion to be at least 200, i.e., a virtually irreversible reaction. Consistent with an earlier report, the data at lower pH and in the absence of NaCl are different and suggest the existence of a second L species; we propose that it is in equilibrium with M2.     

Crystallographic structure of the retinal and the protein after deprotonation of the Schiff base: the switch in the bacteriorhodopsin photocycle

We illuminated bacteriorhodopsin crystals at 210K to produce, in a photostationary state with 60% occupancy, the earliest M intermediate (M1) of the photocycle. The crystal structure of this state was then determined from X-ray diffraction to 1.43 A resolution. When the refined model is placed after the recently determined structure for the K intermediate but before the reported structures for two later M states, a sequence of structural changes becomes evident in which movements of protein atoms and bound water are coordinated with relaxation of the initially strained photoisomerized 13-cis,15-anti retinal. In the K state only retinal atoms are displaced, but in M1 water 402 moves also, nearly 1A away from the unprotonated retinal Schiff base nitrogen. This breaks the hydrogen bond that bridges them, and initiates rearrangements of the hydrogen-bonded network of the extracellular region that develop more fully in the intermediates that follow. In the M1 to M2 transition, relaxation of the C14-C15 and C15=NZ torsion angles to near 180 degrees reorients the retinylidene nitrogen atom from the extracellular to the cytoplasmic direction, water 402 becomes undetectable, and the side-chain of Arg82 is displaced strongly toward Glu194 and Glu204. Finally, in the M2 to M2' transition, correlated with release of a proton to the extracellular surface, the retinal assumes a virtually fully relaxed bent shape, and the 13-methyl group thrusts against the indole ring of Trp182 which tilts in the cytoplasmic direction. Comparison of the structures of M1 and M2 reveals the principal switch in the photocycle: the change of the angle of the C15=NZ-CE plane breaks the connection of the unprotonated Schiff base to the extracellular side and establishes its connection to the cytoplasmic side.     

Structural transition of bacteriorhodopsin is preceded by deprotonation of Schiff base: microsecond time-resolved x-ray diffraction study of purple membrane

The structural changes in the photoreaction cycle of bacteriorhodopsin, a light-driven proton pump, was investigated at a resolution of 7 angstroms by a time-resolved x-ray diffraction experiment utilizing synchrotron x rays from an undulator of SPring-8. The x-ray diffraction measurement system, used in coupling with a pulsed YAG laser, enabled us to record a diffraction pattern from purple membrane film at a time-resolution of 6 micros over the time domain of 5 micros to 500 ms. In the time domain, the functionally most important M-intermediate appears. A series of time-resolved x-ray diffraction data after photo-excitation showed clear intensity changes caused by the conformational changes of helix G in the M-intermediate. The population of the reaction intermediate was prominently observed at approximately 5 ms after a photo-stimulus. In contrast, absorption measurement indicated the deprotonation of the Schiff base predominantly occurred at approximately 300 micros after a photo-stimulus. These results showed that the conformational changes characterizing structurally the M-intermediate predominantly occur at a later stage of the deprotonation of the Schiff base. Thus, the M-intermediate can be divided into two metastable stages with different physical characteristics.     

Effects of individual genetic substitutions of arginine residues on the deprotonation and reprotonation kinetics of the Schiff base during the bacteriorhodopsin photocycle.

The rates are determined for the deprotonation and reprotonation of the protonated Schiff base (PSB) as well as of formation and decay of the UV transient in the photocycle of seven bacteriorhodopsin (bR) mutants in which Arg-7, 82, 164, 175, 225, or 227 are replaced by glutamine and Arg-134 by cysteine. The results show that all these mutations increase the rate of deprotonation of the PSB compared to ebR, (wild-type bacteriorhodopsin expressed in Escherichia coli) greatly increase the rate of the reprotonation of the SB (Schiff base) in the case of the Arg-164 and Arg-175 mutations and dramatically decrease this rate in the case of the Arg-227 mutation. Temperature studies on the latter mutant suggest that the observed change in its rate of reprotonation is due to large decrease in the energy and entropy of activation, similar to those observed for Asp-96 mutations (Miller, A. and D. Orsterhelt. 1990. Biochim. Biophys. Acta. 1020:57-64). These results suggest that the reprotonation process is changed to a proton diffusion-controlled mechanism in the Arg-227 mutant due to a change in the structure of the proton channel. The absorption intensity ratio (AUV/AMslow) of each arginine mutant relative to that of ebR is found to be similar to that for native purple membrane (PM) except for the Arg-227 mutant where it is greatly reduced, and for the Arg-82 mutant where it is not observed, suggesting that both Arg-227 and Arg-82 residues somehow play roles in inducing the UV transient absorption. All the above results are discussed in terms of the model for the structure of bR proposed by Henderson, R., J.M. Baldwin, T.A. Ceska, F. Zemlin, E. Beckmann, and K.H. Downing. (1990. J. Mol. Biol. 213:899-929).     

The protonation-deprotonation kinetics of the protonated Schiff base in bicelle bacteriorhodopsin crystals

In the recently published x-ray crystal structure of the "bicelle" bacteriorhodopsin (bbR) crystal, the protein has quite a different structure from the native and the in cubo bacteriorhodopsin (cbR) crystal. Instead of packing in parallel trimers as do the native membrane and the cbR crystals, in the bbR crystal the protein packs as antiparallel monomers. To date, no functional studies have been performed, to our knowledge, to investigate if the photocycle is observed in this novel protein packing structure. In this study, both Raman and time-resolved transient absorption spectroscopy are used to both confirm the presence of the photocycle and investigate the deprotonation-reprotonation kinetics of the Schiff base proton in the bbR crystal. The observed rates of deprotonation and reprotonation processes of its Schiff base have been compared to those observed for native bR under the same conditions. Unlike the previously observed similarity of the rates of these processes for cbR crystals and those for native bacteriorhodopsin (bR), in bbR crystals the rate of deprotonation has increased by 300%, and the rate of reprotonation has decreased by nearly 700%. These results are discussed in light of the changes observed when native bR is delipidated or monomerized by detergents. Both the change of the hydrophobicity of the environment around the protonated Schiff base and Asp85 and Asp96 (which could change the pKa values of proton donor-acceptor pairs) and the water structure in the bbR crystal are offered as possible explanations for the different observations.     

Alteration of conformation and dynamics of bacteriorhodopsin induced by protonation of Asp 85 and deprotonation of Schiff base as studied by 13C NMR

According to previous X-ray diffraction studies, the D85N mutant of bacteriorhodopsin (bR) with unprotonated Schiff base assumes a protein conformation similar to that in the M photointermediate. We recorded (13)C NMR spectra of [3-(13)C]Ala- and [1-(13)C]Val-labeled D85N and D85N/D96N mutants at ambient temperature to examine how conformation and dynamics of the protein backbone are altered when the Schiff base is protonated (at pH 7) and unprotonated (at pH 10). Most notably, we found that the peak intensities of three to four [3-(13)C]Ala-labeled residues from the transmembrane alpha-helices, including Ala 39, 51, and 53 (helix B) and 215 (helix G), were suppressed in D85N and D85N/D96N both from CP-MAS (cross polarization-magic angle spinning) and DD-MAS (dipolar decoupled-magic angle spinning) spectra, irrespective of the pH. This is due to conformational change and subsequent acquisition of intermediate time-range motions, with correlation times in the order of 10(-)(5) or 10(-)(4) s, which interferes with proton decoupling frequency or frequency of magic angle spinning, respectively, essential for an attempted peak-narrowing to achieve high-resolution NMR signals. Greater changes were achieved, however, at pH 10, which indicate large-amplitude motions of transmembrane helices upon deprotonation of Schiff base and the formation of the M-like state in the absence of illumination. The spectra detected more rapid motions in the extracellular and/or cytoplasmic loops, with correlation times increasing from 10(-)(4) to 10(-)(5) s. Conformational changes in the transmembrane helices were located at helices B, G, and D as viewed from the above-mentioned spectral changes, as well as at 1-(13)C-labeled Val 49 (helix B), 69 (B-C loop), and [3-(13)C]Ala-labeled Ala 126 (D-helix) signals, in addition to the cytoplasmic and extracellular loops. Further, we found that in the M-like state the charged state of Asp 96 at the cytoplasmic side substantially modulated the conformation and dynamics of the extracellular region through long-distance interaction.     

Orientation of the protonated retinal Schiff base group in bacteriorhodopsin from absorption linear dichroism.

Linear dichroism experiments are performed on light-adapted bacteriorhodopsin (BR568) films containing native retinal (A1) and its 3,4-dehydroretinal (A2) analogue to measure the angle between the chromophore transition dipole moment and the membrane normal. QCFF/pi calculations show that the angle between the transition moment and the long axis of the polyene is changed by 3.4 degrees when the C3-C4 bond is unsaturated. The difference vector between the two transition moments points in the same direction as the Schiff base (N----H) bond for the all-trans BR568 chromophore. Because the plane of the chromophore is perpendicular to the membrane plane, a comparison of the transition moment orientations in the A1- and A2-pigments enables us to determine the orientation of the N----H bond with respect to the absolute chromophore (N----C5 vector) orientation. The angles of the transition moments are 70.3 degrees +/- 0.4 degrees and 67.8 degrees +/- 0.4 degrees for the A1- and A2-pigments, respectively. The fact that the change in the transition moment angle (2.5 degrees) is close to the predicted 3.4 degrees supports the idea that the chromophore plane is nearly perpendicular to the membrane plane. The decreased transition moment angle in the A2-analogue requires that the N----H bond and the N----C5 vector point toward the same membrane surface. Available results indicate that the N----C5 vector points toward the exterior in BR568. With this assignment, we conclude that the N----H bond points toward the exterior surface and its most likely counterion Asp-212. This information makes possible the construction of a computer graphics model for the active site in BR568.     

Octopus photoreceptor membranes. Surface charge density and pK of the Schiff base of the pigments.

The chromophore of octopus rhodopsin is 11-cis retinal, linked via a protonated Schiff base to the protein backbone. Its stable photoproduct, metarhodopsin, has all-trans retinal as its chromphore. The Schiff base of acid metarhodopsin (lambda max = 510 nm) is protonated, whereas that of alkaline metarhodopsin (lambda max = 376 nm) is unprotonated. Metarhodopsin in photoreceptor membranes was titrated and the apparent pK of the Schiff base was measured at different ionic strengths. From these salt-dependent pKs the surface charge density of the octopus photoreceptor membranes and the intrinsic Schiff base pK of metarhodopsin were obtained. The surface charge density is sigma = -1.6 +/- 0.1 electronic charges per 1,000 A2. Comparison of the measured surface charge density with values from octopus rhodopsin model structures suggests that the measured value is for the extracellular surface and so the Schiff base in metarhodopsin is freely accessible to protons from the extracellular side of the membrane. The intrinsic Schiff base pK of metarhodopsin is 8.44 +/- 0.12, whereas that of rhodopsin is found to be 10.65 +/- 0.10 in 4.0 M KCl. These pK values are significantly higher than the pK value around 7.0 for a retinal Schiff base in a polar solvent; we suggest that a plausible mechanism to increase the pK of the retinal pigments is the preorganization of their chromophore-binding sites. The preorganized site stabilizes the protonated Schiff base with respect to the unprotonated one. The difference in the pK for the octopus rhodopsin compared with metarhodopsin is attributed to the relative freedom of the latter's chromophore-binding site to rearrange itself after deprotonation of the Schiff base.     

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.     

Light activation of the isomerization and deprotonation of the protonated Schiff base retinal

We perform an ab initio analysis of the photoisomerization of the protonated Schiff base of retinal (PSB-retinal) from 11-cis to 11-trans rotating the C10-C11=C12-C13 dihedral angle from 0° (cis) to -180° (trans). We find that the retinal molecule shows the lowest rotational barrier (0.22 eV) when its charge state is zero as compared to the barrier for the protonated molecule which is ∼0.89 eV. We conclude that rotation most likely takes place in the excited state of the deprotonated retinal. The addition of a proton creates a much larger barrier implying a switching behavior of retinal that might be useful for several applications in molecular electronics. All conformations of the retinal compound absorb in the green region with small shifts following the dihedral angle rotation; however, the Schiff base of retinal (SB-retinal) at trans-conformation absorbs in the violet region. The rotation of the dihedral angle around the C11=C12 π-bond affects the absorption energy of the retinal and the binding energy of the SB-retinal with the proton at the N-Schiff; the binding energy is slightly lower at the trans-SB-retinal than at other conformations of the retinal.     

Protein changes associated with reprotonation of the Schiff base in the photocycle of Asp96-->Asn bacteriorhodopsin. The MN intermediate with unprotonated Schiff base but N-like protein structure.

The difference Fourier transform infrared spectrum for the N intermediate in the photoreaction of the light-adapted form of bacteriorhodopsin can be recorded at pH 10 at 274 K (Pfefferlé, J.-M., Maeda, A., Sasaki, J., and Yoshizawa, T. (1991) Biochemistry 30, 6548-6556). Under these conditions, Asp96-->Asn bacteriorhodopsin gives a photoproduct which shows changes in protein structure similar to those observed in N of wild-type bacteriorhodopsin. However, decreased intensity of the chromophore bands and the single absorbance maximum at about 400 nm indicate that the Schiff base is unprotonated, as in the M intermediate. This photoproduct was named MN. At pH 7, where the supply of proton is not as restricted as at pH 10, Asp96-->Asn bacteriorhodopsin yields N with a protonated Schiff base. The Asn96 residue, which cannot deprotonate as Asp96 in wild-type bacteriorhodopsin, is perturbed upon formation of both MN at pH 10 and N at pH 7. We suggest that the reprotonation of the Schiff base is preceded by a large change in the protein structure including perturbation of the residue at position 96.     

Deprotonation of the Schiff base of bacteriorhodopsin is obligate in light-induced proton pumping

Bacteriorhodopsin (bR) in purple membranes was permethylated with formaldehyde and pyridine-borane with the incorporation of approximately 12 methyl groups. This new pigment, PMbR, absorbed light in the dark-adapted state with a lambda max at 558 nm, virtually the same as that of bR. Light adaptation of PMbR produced a lambda max of 564 nm with a slightly elevated epsilon. Similar changes occurred with bR. When incorporated into asolectin vesicles, PMbR was able to pump protons in the light with an efficiency similar to that of bR itself. Bleaching of PMbR exposed its active site lysine residue, which was monomethylated to form active site methylated bR (AMbR) after regeneration with all-trans-retinal. This blue pigment, which is a cyanopsin rather than a rhodopsin, showed an extraordinary red shift, absorbing light with a lambda max of 620 nm in the dark-adapted state. Light adaptation of AMbR resulted in a spectral shift to 616 nm with a decrease in epsilon. This change was completely reversible in the dark. This shift was interpreted to mean that an L-like intermediate was accumulating, as would be expected if deprotonation of the protonated Schiff base could not occur to produce the M intermediate. Furthermore, when incorporated into asolectin vesicles, AMbR proved incapable of pumping protons in the light. It was concluded from these experiments that deprotonation of the Schiff base of bR is obligate for light-induced proton pumping.     

FTIR studies of internal water molecules in the Schiff base region of bacteriorhodopsin

In a light-driven proton pump protein, bacteriorhodopsin (BR), three water molecules participate in a pentagonal cluster that stabilizes an electric quadrupole buried inside the protein. Previously, low-temperature Fourier-transform infrared (FTIR) difference spectra between BR and the K photointermediate in D(2)O revealed six O-D stretches of water in BR at 2690, 2636, 2599, 2323, 2292, and 2171 cm(-)(1), while five water bands were observed at 2684, 2675, 2662, 2359, and 2265 cm(-)(1) for the K intermediate. The frequencies are widely distributed over the possible range of stretching vibrations of water, and water molecules at <2400 cm(-)(1) were suggested to hydrate negative charges because of their extremely strong hydrogen bonds. In this paper, we aimed to reveal the origin of these water bands in the K minus BR spectra by use of various mutant proteins. The water bands were not affected by the mutations at the cytoplasmic side, such as T46V, D96N, and D115N, implying that the water molecules in the cytoplasmic domain do not change their hydrogen bonds in the BR to K transition. In contrast, significant modifications of the water bands were observed for the mutations in the Schiff base region and at the extracellular side, such as R82Q, D85N, T89A, Y185F, D212N, R82Q/D212N, and E204Q. From these results, we concluded that the six O-D stretches of BR originate from three water molecules, water401, -402, and -406, involved in the pentagonal cluster. Two stretching modes of each water molecule are highly separate (300-470 cm(-)(1) for O-D stretches and 500-770 cm(-)(1) for O-H stretches), which is consistent with the previous QM/MM calculation. The small amplitudes of vibrational coupling are presumably due to strong association of the waters to negative charges of Asp85 and Asp212. Among various mutant proteins, only D85N and D212N lack strongly hydrogen-bonded water molecules (<2400 cm(-)(1)) and proton pumpimg activity. We thus infer that the presence of a strong hydrogen bond of water is a prerequisite for proton pumping in BR. Internal water molecules in such a specific environment are discussed in terms of functional importance for rhodopsins.     

Chloride binding regulates the Schiff base pK in gecko P521 cone-type visual pigment

The binding of chloride is known to shift the absorption spectrum of most long-wavelength-absorbing cone-type visual pigments roughly 30 nm to the red. We determined that the chloride binding constant for this color shift in the gecko P521 visual pigment is 0.4 mM at pH 6.0. We found an additional effect of chloride on the P521 pigment: the apparent pKa of the Schiff base in P521 is greatly increased as the chloride concentration is increased. The apparent Schiff base pKa shifts from 8.4 for the chloride-free form to >10.4 for the chloride-bound form. We show that this shift is due to chloride binding to the pigment, not to the screening of the membrane surface charges by chloride ions. We also found that at high pH, the absorption maximum of the chloride-free pigment shifts from 495 to 475 nm. We suggest that the chloride-dependent shift of the apparent Schiff base pKa is due to the deprotonation of a residue in the chloride binding site with a pKa of ca. 8.5, roughly that of the Schiff base in the absence of chloride. The deprotonation of this site results in the formation of the 475 nm pigment and a 100-fold decrease in the pigment's ability to bind chloride. Increasing the concentration of chloride results in the stabilization of the protonated state of this residue in the chloride binding site and thus increased chloride binding with an accompanying increase in the Schiff base pK.     

Water is required for proton transfer from aspartate-96 to the bacteriorhodopsin Schiff base.

During the M in equilibrium with N----BR reaction sequence in the bacteriorhodopsin photocycle, proton is exchanged between D96 and the Schiff base, and D96 is reprotonated from the cytoplasmic surface. We probed these and the other photocycle reactions with osmotically active solutes and perturbants and found that the M in equilibrium with N reaction is specifically inhibited by withdrawing water from the protein. The N----BR reaction in the wild-type protein and the direct reprotonation of the Schiff base from the cytoplasmic surface in the site-specific mutant D96N are much less affected. Thus, it appears that water is required inside the protein for reactions where a proton is separated from a buried electronegative group, but not for those where the rate-limiting step is the capture of a proton at the protein surface. In the wild type, the largest part of the barrier to Schiff base reprotonation is the enthalpy of separating the proton from D96, which amounts to about 40 kJ/mol. We suggest that in spite of this D96 confers an overall kinetic advantage because when this residue becomes anionic in the N state its electric field near the cytoplasmic surface lowers the free energy barrier of the capture of a proton in the next step. In the D96N protein, the barrier to the M----BR reaction is 20 kJ/mol higher than what would be expected from the rates of the M----N and N----BR partial reactions in the wild type, presumably because this mechanism is not available.     

Titration of the bacteriorhodopsin Schiff base involves titration of an additional protein residue

The retinal protein protonated Schiff base linkage plays a key role in the function of bacteriorhodopsin (bR) as a light-driven proton pump. In the unphotolyzed pigment, the Schiff base (SB) is titrated with a pK(a) of approximately 13, but following light absorption, it experiences a decrease in the pK(a) and undergoes several alterations, including a deprotonation process. We have studied the SB titration using retinal analogues which have intrinsically lower pK(a)'s which allow for SB titrations over a much lower pH range. We found that above pH 9 the channel for the SB titration is perturbed, and the titration rate is considerably reduced. On the basis of studies with several mutants, it is suggested that the protonation state of residue Glu204 is responsible for the channel perturbation. We suggest that above pH 12 a channel for the SB titration is restored probably due to titration of an additional protein residue. The observations may imply that during the bR photocycle and M photointermediate formation the rate of Schiff base protonation from the bulk is decreased. This rate decrease may be due to the deprotonation process of the "proton-releasing complex" which includes Glu204. In contrast, during the lifetime of the O intermediate, the protonated SB is exposed to the bulk. Possible implications for the switch mechanism, and the directionality of the proton movement, are discussed.