Kinetics and pH dependence of light-induced deprotonation of the Schiff base of rhodopsin: possible coupling to proton uptake and formation of the active form of Meta II.

In this paper we first review what is known about the kinetics of Meta II formation, the role and stoichiometry of protons in Meta II formation, the kinetics of the light-induced changes of proton concentration, and the site of proton uptake. We then go on to compare the processes that lead to the deprotonation of the Schiff base in bacteriorhodopsin with rhodopsin. We point out that the similarity of the signs of the light-induced electrical signals from the two kinds of oriented pigment molecules could be explained by bacteriorhodopsin releasing a proton from its extracellular side while rhodopsin taking up a proton on its cytoplasmic side. We then examined the pH dependence of both the absorption spectrum of the unphotolyzed state and the amplitude and kinetics of Meta II formation in bovine rhodopsin. We also measured the effect of deuteration and azide on Meta II formation. We concluded that the pKa of the counter-ion to the Schiff base of bovine rhodopsin and of a surface residue that takes up a proton upon photolysis are both less than 4 in the unphotolyzed state. The data on pH dependence of Meta II formation indicated that the mechanisms involved are more complicated than just two sequential, isospectral forms of Meta II in the bleaching sequence. Finally we examined the evidence that, like in bacteriorhodopsin, the protonation of the Schiff bases's counter-ion (Glu113) is coupled to the changing of the pKa of a protonatable surface group, called Z for rhodopsin and tentatively assigned to Glu134. We conclude that there probably is such a coupling, leading to the formation of the active form of Meta II.

Exploring the function of Tyr83 in bacteriorhodopsin: features of the Y83F and Y83N mutants.

Tyrosine-83, a residue which is conserved in all halobacterial retinal proteins, is located at the extracellular side in helix C of bacteriorhodopsin. Structural studies indicate that its hydroxyl group is hydrogen bonded to Trp189 and possibly to Glu194, a residue which is part of the proton release complex (PRC) in bacteriorhodopsin. To elucidate the role of Tyr83 in proton transport, we studied the Y83F and Y83N mutants. The Y83F mutation causes an 11 nm blue shift of the absorption spectrum and decreases the size of the absorption changes seen upon dark adaptation. The light-induced fast proton release, which accompanies formation of the M intermediate, is observed only at pH above 7 in Y83F. The pK(a) of the PRC in M is elevated in Y83F to about 7.3 (compared to 5.8 in WT). The rate of the recovery of the initial state (the rate of the O --> BR transition) and light-induced proton release at pH below 7 is very slow in Y83F (ca. 30 ms at pH 6). The amount of the O intermediate is decreased in Y83F despite the longer lifetime of O. The Y83N mutant shows a similar phenotype in respect to proton release. As in Y83F, the recovery of the initial state is slowed several fold in Y83N. The O intermediate is not seen in this mutant. The data indicate that the PRC is functional in Y83F and Y83N but its pK(a) in M is increased by about 1.5 pK units compared to the WT. This suggests that Tyr83 is not the main source for the proton released upon M formation in the WT; however, Tyr83 is involved in the proton release affecting the pK(a) of the PRC in M and the rate of proton transport from Asp85 to PRC during the O --> bR transition. Both the Y83F and the Y83N mutations lead to a greatly decreased functionality of the pigment at high pH because most of the pigment is converted into the inactive P480 species, with a pK(a) 8-9.

Trapping and spectroscopic identification of the photointermediates of bacteriorhodopsin at low temperatures.

Light-driven transmembrane proton pumping by bacteriorhodopsin occurs in the photochemical cycle, which includes a number of spectroscopically identifiable intermediates. The development of methods to crystallize bacteriorhodopsin have allowed it to be studied with high-resolution X-ray diffraction, opening the possibility to advance substantially our knowledge of the structure and mechanism of this light-driven proton pump. A key step is to obtain the structures of the intermediate states formed during the photocycle of bacteriorhodopsin. One difficulty in these studies is how to trap selectively the intermediates at low temperatures and determine quantitatively their amounts in a photosteady state. In this paper we review the procedures for trapping the K, L, M and N intermediates of the bacteriorhodopsin photocycle and describe the difference absorption spectra accompanying the transformation of the all-trans-bacteriorhodopsin into each intermediate. This provides the means for quantitative analysis of the light-induced mixtures of different intermediates produced by illumination of the pigment at low temperatures.

Relocation of internal bound water in bacteriorhodopsin during the photoreaction of M at low temperatures: an FTIR study.

Changes in the FTIR difference spectra upon photoconversion of the M intermediate to its photoproduct(s) M' were studied in wild-type bacteriorhodopsin and several mutants at low temperatures. The studies aimed at examining whether internally bound water molecules interact with the chromophore and the key residues Asp85 and Asp96 in M, and whether these water molecules participate in the reprotonation of the Schiff base. We have found that three water molecules are perturbed by the isomerization of the chromophore in the M --> M' transition at 80 K. The perturbation of one water molecule, detected as a bilobe at 3567(+)/3550(-) cm(-)(1), relaxed in parallel with the relaxation of an Asp85 perturbation upon increasing temperature from 80 to 100 and 133 K (before the reprotonation of the Schiff base). Two water bands of M at 3588 and 3570 cm(-)(1) shift to 3640 cm(-)(1) upon photoconversion at 173 K. These bands were attributed to water molecules which are located in the vicinity of the Schiff base and Asp85 (Wat85). In the M to M' transition at 80 and 100 K, where the Schiff base remained unprotonated, the Wat85 pair stayed in similar states to those in M. The reprotonation of the Schiff base at 133 K occurred without the restoration of the Wat85 band around 3640 cm(-)(1). This band was restored at higher temperatures. Two water molecules in the region surrounded by Thr46, Asp96, and Phe219 (Wat219) were perturbed in the M to M' transition at 80 K and relaxed in parallel with the relaxation of the perturbation of Asp96 upon increasing the temperature. Mutant studies show that upon photoisomerization of the chromophore at 80 K one of the Wat219 water molecules moves closer to Val49 (located near the lysine side chain attached to retinal, and close to the Schiff base). These data along with our previous results indicate that the water molecules in the cytoplasmic domain participate in the connection of Asp96 with the Schiff base and undergo displacement during photoconversions, presumably shuttling between the Schiff base and a site close to Asp96 in the L to M to N transitions.

Evidence for the rate of the final step in the bacteriorhodopsin photocycle being controlled by the proton release group: R134H mutant.

Light absorbed by bacteriorhodopsin (bR) leads to a proton being released at the extracellular surface of the purple membrane. Structural studies as well as studies of mutants of bR indicate that several groups form a pathway for proton transfer from the Schiff base to the extracellular surface. These groups include D85, R82, E204, E194, and water molecules. Other residues may be important in tuning the initial state pK(a) values of these groups and in mediating light-induced changes of the pK(a) values. A potentially important residue is R134: it is located close to E194 and might interact electrostatically to affect the pK(a) of E194 and light-induced proton release. In this study we investigated effects of the substitution of R134 with a histidine on light-induced proton release and on the photocycle transitions associated with proton transfer. By measuring the light-induced absorption changes versus pH, we found that the R134H mutation results in an increase in the pK(a) of the proton release group in both the M (0.6 pK unit) and O (0.7 pK unit) intermediate states. This indicates the importance of R134 in tuning the pK(a) of the group that, at neutral and high pH, releases the proton upon M formation (fast proton release) and that, at low pH, releases the proton simultaneously with O decay (slow proton release). The higher pK(a) of the proton release group found in R134H correlates with the slowing of the rate of the O --> bR transition at low pH and probably is the cause of this slowing. The pH dependence of the fraction of the O intermediate is altered in R134H compared to the WT but is similar to that in the E194D mutant: a very small amount of O is present at neutral pH, but the fraction of O increases greatly upon decreasing the pH. These results provide further support for the hypothesis that the O --> bR transition is controlled by the rate of deprotonation of the proton release group. These data also provide further evidence for the importance of the R134-E194 interaction in modulating proton release from D85 after light has led to its being protonated.

pKa of the protonated Schiff base of visual pigments.

The pKa of bovine rhodopsin is greater than 15; that of the long-wave-length-sensitive gecko P521 pigment ranges from 8.4 to 10.5 depending on chloride concentration; and that of octopus, an invertebrate, is 10.5. These pKa values are much higher than are needed just to maintain the Schiff base in its protonated state in the photoreceptor cell. The high pKa of the Schiff base may be at least partially related to a low pKa of its counterion, which would lower the frequency of thermal isomerization of the chromophore and thus lower the dark noise in the photoreceptor cell. After light absorption, the high pKa of the protonated Schiff base of a vertebrate visual pigment must get lowered enough to allow it to deprotonate, a required step in vertebrate visual excitation. This deprotonation step is not required in invertebrate visual excitation.

Two groups control light-induced Schiff base deprotonation and the proton affinity of Asp85 in the Arg82 his mutant of bacteriorhodopsin.

Arg(82) is one of the four buried charged residues in the retinal binding pocket of bacteriorhodopsin (bR). Previous studies show that Arg(82) controls the pK(a)s of Asp(85) and the proton release group and is essential for fast light-induced proton release. To further investigate the role of Arg(82) in light-induced proton pumping, we replaced Arg(82) with histidine and studied the resulting pigment and its photochemical properties. The main pK(a) of the purple-to-blue transition (pK(a) of Asp(85)) is unusually low in R82H: 1.0 versus 2.6 in wild type (WT). At pH 3, the pigment is purple and shows light and dark adaptation, but almost no light-induced Schiff base deprotonation (formation of the M intermediate) is observed. As the pH is increased from 3 to 7 the M yield increases with pK(a) 4.5 to a value approximately 40% of that in the WT. A transition with a similar pK(a) is observed in the pH dependence of the rate constant of dark adaptation, k(da). These data can be explained, assuming that some group deprotonates with pK(a) 4.5, causing an increase in the pK(a) of Asp(85) and thus affecting k(da) and the yield of M. As the pH is increased from 7 to 10.5 there is a further 2.5-fold increase in the yield of M and a decrease in its rise time from 200 micros to 75 micros with pK(a) 9. 4. The chromophore absorption band undergoes a 4-nm red shift with a similar pK(a). We assume that at high pH, the proton release group deprotonates in the unphotolyzed pigment, causing a transformation of the pigment into a red-shifted "alkaline" form which has a faster rate of light-induced Schiff base deprotonation. The pH dependence of proton release shows that coupling between Asp(85) and the proton release group is weakened in R82H. The pK(a) of the proton release group in M is 7.2 (versus 5.8 in the WT). At pH < 7, most of the proton release occurs during O --> bR transition with tau approximately 45 ms. This transition is slowed in R82H, indicating that Arg(82) is important for the proton transfer from Asp(85) to the proton release group. A model describing the interaction of Asp(85) with two ionizable residues is proposed to describe the pH dependence of light-induced Schiff base deprotonation and proton release.

Chromophore-protein-water interactions in the L intermediate of bacteriorhodopsin: FTIR study of the photoreaction of L at 80 K.

Using FTIR spectroscopy, perturbations of several residues and internal water molecules have been detected when light transforms all-trans bacteriorhodopsin (BR) to its L intermediate having a 13-cis chromophore. Illumination of L at 80 K results in an intermediate L' absorbing around 550 nm. L' thermally converts to the original BR only at >130 K. In this study, we used the light-induced transformation of L to L' at 80 K to identify some amino acid residues and water molecules that closely interact with the chromophore and distinguish them from those residues not affected by the photoreaction. The L minus L' FTIR difference spectrum shows that the chromophore in L' is in the all-trans configuration. The perturbed states of Asp96 and Val49 and of the environment along the aliphatic part of the retinal and Lys216 seen in L are not affected by the L --> L' photoreaction. On the other hand, the environments of the Schiff base of the chromophore, of Asp115, and of water molecules close to Asp85 returned in L' to their state in which they originally had existed in BR. The water molecules that are affected by the mutations of Thr46 and Asp96 also change to a different state in the L --> L' transition, as indicated by transformation of a water O-H vibrational band at 3497 cm-1 in L into an intense peak at 3549 cm-1 in L'. Notably, this change of water bands in the L --> L' transition at 80 K is entirely different from the changes observed in the BR --> K photoreaction at the same temperature, which does not show such intense bands. These results suggest that these water molecules move closer to the Schiff base as a hydrogen bonding cluster in L and L', presumably to stabilize its protonated state during the BR to L transition. They may contribute to the structural constraints that prevent L from returning to the initial BR upon illumination at 80 K.

How vertebrate and invertebrate visual pigments differ in their mechanism of photoactivation.

In vertebrate visual pigments, a glutamic acid serves as a negative counterion to the positively charged chromophore, a protonated Schiff base of retinal. When photoisomerization leads to the Schiff base deprotonating, the anionic glutamic acid becomes protonated, forming a neutral species that activates the visual cascade. We show that in octopus rhodopsin, the glutamic acid has no anionic counterpart. Thus, the "counterion" is already neutral, so no protonated form of an initially anionic group needs to be created to activate. This helps to explain another observation-that the active photoproduct of octopus rhodopsin can be formed without its Schiff base deprotonating. In this sense, the mechanism of light activation of octopus rhodopsin is simpler than for vertebrates, because it eliminates one of the steps required for vertebrate rhodopsins to achieve their activating state.

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.

The proton release group of bacteriorhodopsin controls the rate of the final step of its photocycle at low pH.

The factors determining the pH dependence of the formation and decay of the O photointermediate of the bacteriorhodopsin (bR) photocycle were investigated in the wild-type (WT) pigment and in the mutants of Glu-194 and Glu-204, key residues of the proton release group (PRG) in bR. We have found that in the WT the rate constant of O --> bR transition decreases 30-fold upon decreasing the pH from 6 to 3 with a pKa of about 4.3. D2O slows the rise and decay of the O intermediate in the WT at pH 3.5 by a factor of 5.5. We suggest that the rate of the O --> bR transition (which reflects the rate of deprotonation of the primary proton acceptor Asp-85) at low pH is controlled by the deprotonation of the PRG. To test this hypothesis, we studied the E194D mutant. We show that the pKa of the PRG in the ground state of the E194D mutant, when Asp-85 is protonated, is increased by 1.2 pK units compared to that of the WT. We found a similar increase in the pKa of the rate constant of the O --> bR transition in E194D. This provides further evidence that the rate of the O --> bR transition is controlled by the PRG. In a further test, the E194Q mutation, which disables the PRG and slows proton release, almost completely eliminates the pH dependence of O decay at pHs below 6. A second phenomenon we investigated was that in the WT at neutral and alkaline pH the fraction of the O intermediate decreases with pKa 7.5. A similar pH dependence is observed in the mutants in which the PRG is disabled, E194Q and E204Q, suggesting that the decrease in the fraction of the O intermediate with pKa ca. 7.5 is not controlled by the PRG. We propose that the group with pKa 7.5 is Asp-96. The slowing of the reprotonation of Asp-96 at high pH is the cause of the decrease in the rate of the N --> O transition, leading to the decrease in the fraction of O.

The unique lipid composition of gecko (Gekko Gekko) photoreceptor outer segment membranes.

This study investigated the lipid and fatty acid composition of gecko photoreceptor outer segment membranes which contain the P521 cone-type pigment. The lipids of gecko photoreceptor outer segment membranes were first extracted and separated by thin layer chromatography (TLC) and then analyzed by gas chromatography (GC). Our results show that gecko photoreceptor outer segment membranes contain less phosphatidylethanolamine (PE) and more phosphatidylcholine (PC) and phosphatidylserine (PS) compared with those of bovine and frog. The content of the polyunsaturated fatty acid, docosahexaenoic acid (DHA), in PC and PS is also the highest yet reported (55 and 63%, respectively). These lipid differences may provide some insight into the specific lipid requirements of cone-type pigments.

Early photolysis intermediates of gecko and bovine artificial visual pigments.

Nanosecond laser photolysis measurements were conducted on digitonin extracts of artificial pigments prepared from the cone-type visual pigment, P521, of the Tokay gecko (Gekko gekko) retina. Artificial pigments were prepared by regeneration of bleached gecko photoreceptor membranes with 9-cis-retinal, 9-cis-14-methylretinal, or 9-cis-alpha-retinal. Absorbance difference spectra were recorded at a sequence of time delays from 30 ns to 60 microseconds following excitation with a pulse of 477-nm actinic light. Global analysis showed the kinetic data for all three artificial gecko pigments to be best fit by two-exponential processes. These two-exponential decays correspond to similar decays observed after photolysis of P521 itself, with the first process being the decay of the equilibrated P521 Batho<-->P521 BSI mixture to P521 Lumi and the second process being the decay of P521 Lumi to P521 Meta I. In spite of its large blue shift relative to P521, iso-P521 displays a normal chloride depletion induced blue shift. Iso-P521's early intermediates up to Lumi were also blue-shifted, with the P521 Batho<-->P521 BSI equilibrated mixture being 15 nm blue-shifted and P521 Lumi being 8 nm blue-shifted relative to the intermediates formed after P521 photolysis. The blue shift associated with the iso-pigment is reduced or disappears entirely by P521 Meta I. Similar blue shifts were observed for the early intermediates observed after photolysis of bovine isorhodopsin, with the Lumi intermediate blue-shifted 5 nm compared to the Lumi intermediate formed after photolysis of bovine rhodopsin. These shifts indicate that a difference exists between the binding sites of 9- and 11-cis pigments which persists for microseconds at 20 degrees C.

Glutamate-194 to cysteine mutation inhibits fast light-induced proton release in bacteriorhodopsin.

Substitution of glutamic acid-194, a residue on the extracellular surface of bacteriorhodopsin, with a cysteine inhibits the fast light-induced proton release that normally is coupled with the deprotonation of the Schiff base during the L to M transition. Proton release in this mutant occurs at the very end of the photocycle and coincides with deprotonation of the primary proton acceptor, Asp-85, during the O to bR transition. the E194C mutation also results in a slowing down of the photocycle by about 1 order of magnitude as compared to the wild type and produces a strong effect on the pH dependence of dark adaptation that is interpreted as a drastic reduction or elimination of the coupling between the primary proton acceptor Asp-85 and the proton release group. These data indicate that Glu-194 is a critical component of the proton release complex in bacteriorhodopsin.

Charge movements in the 13-cis photocycles of the bacteriorhodopsin mutants R82K and R82Q.

We have examined light-induced currents in oriented membranes of the bacteriorhodopsin mutants R82K and R82Q. Our results suggest that two photocurrent components found in R82K, with 30 and 300 microseconds lifetimes, are due to the photocycle of the 13-cis rather than the all-trans form of the pigment. We investigated the pH dependence of these components and their correspondence to absorbance changes at 660 nm characteristic of photointermediates of the 13-cis cycle. The presence of a D2O effect suggests that the charge motions producing these photocurrents are related to proton or protonated amino acid movement within the molecule. The current amplitudes depend on the protonation states of at least two residues, D85 and (probably) E204. In R82Q, a 10 microseconds photocurrent is observed that also depends on the protonation state of D85 and is similar to the 30 microseconds current in R82K. We attempt to explain these currents in terms of a model for interacting residues in the extracellular half of the bacteriorhodopsin channel.

Proton uptake and release are rate-limiting steps in the photocycle of the bacteriorhodopsin mutant E204Q.

In the absence of the putative proton release group, E204, the second half of the photocycle of the E204Q mutant of bacteriorhodopsin is slowed down more than 10-fold compared to the wild type. The effects of pH and D2O on the M decay and O formation rates in E204Q suggest that proton uptake occurs concurrently with the N <--> O transition, possibly coupled with the thermal reisomerization of the retinal. Hence, one of the rate-limiting steps in the slow E204Q photocycle is proton uptake from the outside medium, coincident with the decay of the slow component of M (the N <--> O transition). The second rate-limiting step is the long lifetime of decay of the O state, due to a high activation barrier for the deprotonation of D85 in the O --> bR step of the E204Q photocycle. Addition of the weakly acidic anions azide, cyanate, or formate accelerates the decay of the O intermediate, and restores the total photocycling time to that observed in the wild-type pigment, by accelerating the deprotonation of D85. We also find that azide similarly accelerates the decay of O in the wild type under conditions in which E204 does not deprotonate during the photocycle (pH < 6). It has previously been shown that azide and other weak acids can influence proton transfers in the cytoplasmic half of the protein [Tittor, J., Soell, C., Oesterhelt, D., Butt, H.-J., & Bamberg, E. (1989) EMBO J. 8, 3477-3482]; we suggest that these weak acids can affect proton transfers in the extracellular half of the protein as well.

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.

Mutation of arginine 134 to lysine alters the pK(a)s of key groups involved in proton pumping by bacteriorhodopsin.

Arginine 134 is located near the extracellular surface of bacteriorhodopsin (bR) and may interact with one or more nearby glutamate residues. In the bR mutant R134K, light-induced Schiff-base deprotonation (formation of the M intermediate) exhibits several kinetic components and has a complex pH dependence. The kinetics and pH dependence of M formation were analyzed using the following general guidelines for interpreting M formation: (1) The fastest component of M formation reflects the redistribution of the Schiff-base proton to D85, the usual proton acceptor, in response to the change in the proton affinities of the Schiff base and D85 early in the photocycle; (2) Two additional components of M formation reflect transitions between spectroscopically similar substates of M. By applying these guidelines, supplemented by information about the pK(a)s of D85 and the proton release group from acid (purple-to-blue) and alkaline titrations of the absorption spectra of the unphotolyzed R134K pigment, we explain the pH dependence of M formation as being due to titration of the counterion, D85, and of the proton release group. We calculate, in R134K, that the pKa of D85 is 4.6 in the unphotolyzed state, while the pKa of the proton release group is 8.0 in the unphotolyzed state but drops to approximately 5.8 in the M intermediate. The same value for the pKa of the proton release group in the M intermediate is obtained when we use photocurrent measurements to monitor proton release. The altered values of these pK(a)s relative to the corresponding values in wild-type bR suggest that D85 and the proton release group are coupled more weakly in R134K than in the wild type.

Evidence that aspartate-85 has a higher pK(a) in all-trans than in 13-cisbacteriorhodopsin.

Three experimental observations indicate that the pK(a) of the purple-to-blue transition (the pK(a) of Asp-85) is higher for all-trans-bR(1) than for 13-cis-bR. First, light adaptation of bacteriorhodopsin (bR) at pHs near the pK(a) of Asp-85 causes an increase in the fraction of the blue membrane present. This transformation is reversible in the dark. Second, the pK(a) of the purple-to-blue transition in the dark is lower than that in the light-adapted bR (pK(a)(DA) = 3.5, pK(a)(LA) = 3.8 in 10 microM K(2)SO(4)). Third, the equilibrium fractions of 13-cis and all-trans isomers are pH dependent; the fraction of all-trans-bR increases upon formation of the blue membrane. Based on the conclusion that thermal all-trans <=> 13-cis isomerization occurs in the blue membrane rather than in the purple, we have developed a simple model that accounts for all three observations. From the fit of experimental data we estimate that the pK(a) of Asp-85 in 13-cis-bR is 0.5 +/- 0.1 pK(a) unit less than the pK(a) of all-trans-bR. Thus in 10 microM K(2)SO(4), pK(a)(c) = 3.3, whereas pK(a)(t) = 3.8.