Proton translocation by bacteriorhodopsin in the absence of substantial conformational changes

Unlike wild-type bacteriorhodopsin (BR), the BR triple mutant D96G/F171C/F219L has been shown to undergo only minor structural rearrangements during its photocycle. Nonetheless, the mutant is capable of transporting protons at a rate of 125(+/-40) H+/BR per minute under light-saturating conditions. Light adaptation of the triple mutant's retinal proceeds in a pH-dependent manner up to a maximum of 63% all-trans. These two findings imply that the transport activity of the triple mutant comprises 66% of the wild-type activity. Time-resolved spectroscopy reveals that the identity and sequence of intermediates in the photocycle of the triple mutant in the all-trans configuration correspond to that of wild-type BR. The only differences relate to a slower rise and decay of the M and O intermediates, and a significant spectral contribution from a 13-cis component. No indication for accumulation of the N intermediate is found under a variety of conditions that normally favor the formation of this species in wild-type BR. The Fourier transform infrared (FTIR) spectrum of the M intermediate in the triple mutant resembles that of wild type. Minor changes in the amide I region during the photocycle suggest that only small movements of the protein backbone occur. Electron microscopy reveals large differences in conformation between the unilluminated state of the mutant protein and wild-type but no light-induced changes in time-resolved measurements. Evidently, proton transport by the triple mutant does not require the major conformational rearrangements that occur on the same time-scale with wild-type. Thus, we conclude that large conformational changes observed in the photocycle of the wild-type and many BR mutants are not a prerequisite for the change in accessibility of the Schiff base nitrogen atom that must occur during vectorial catalysis to allow proton transport.     

Proton Transfer to Flavin Stabilizes the Signaling State of the Blue Light Receptor Plant Cryptochrome

Plant cryptochromes regulate the circadian rhythm, flowering time, and photomorphogenesis in higher plants as responses to blue light. In the dark, these photoreceptors bind oxidized FAD in the photolyase homology region (PHR). Upon blue light absorption, FAD is converted to the neutral radical state, the likely signaling state, by electron transfer via a conserved tryptophan triad and proton transfer from a nearby aspartic acid. Here we demonstrate, by infrared and time-resolved UV-visible spectroscopy on the PHR domain, that replacement of the aspartic acid Asp-396 with cysteine prevents proton transfer. The lifetime of the radical is decreased by 6 orders of magnitude. This short lifetime does not permit to drive conformational changes in the C-terminal extension that have been associated with signal transduction. Only in the presence of ATP do both the wild type and mutant form a long-lived radical state. However, in the mutant, an anion radical is formed instead of the neutral radical, as found previously in animal type I cryptochromes. Infrared spectroscopic experiments demonstrate that the light-induced conformational changes of the PHR domain are conserved in the mutant despite the lack of proton transfer. These changes are not detected in the photoreduction of the non-photosensory d-amino acid oxidase to the anion radical. In conclusion, formation of the anion radical is sufficient to generate a protein response in plant cryptochromes. Moreover, the intrinsic proton transfer is required for stabilization of the signaling state in the absence of ATP.     

Transmembrane charge separation during the ferryl-oxo -> oxidized transition in a nonpumping mutant of cytochrome c oxidase

The N139D mutant of cytochrome c oxidase from Rhodobacter sphaeroides retains full steady state oxidase activity but completely lacks proton translocation coupled to turnover in reconstituted liposomes (Pawate, A. S., Morgan, J., Namslauer, A., Mills, D., Brzezinski, P., Ferguson-Miller, S., and Gennis, R. B. (2002) Biochemistry 41, 13417-13423). Here, time-resolved electron transfer and vectorial charge translocation in the ferryl-oxo --> oxidized transition (transfer of the 4th electron in the catalytic cycle) have been studied with the N139D mutant using ruthenium(II)-tris-bipyridyl complex as a photoactive single-electron donor. With the wild type oxidase, the flash-induced generation of Deltaphi in the ferryl-oxo --> oxidized transition begins with rapid vectorial electron transfer from CuA to heme a (tau approximately 15 micros), followed by two protonic phases, referred to as the intermediate (0.4 ms) and slow electrogenic phases (1.5 ms). In the N139D mutant, only a single protonic phase (tau approximately 0.6 ms) is observed, which was associated with electron transfer from heme a to the heme a3/CuB site and decelerates approximately 4-fold in D2O. With the wild type oxidase, such a high H2O/D2O solvent isotope effect is characteristic of only the slow (1.5 ms) phase. Presumably, the 0.6-ms electrogenic phase in the N139D mutant reports proton transfer from the inner aqueous phase to Glu-286, replacing the "chemical" proton transferred from Glu-286 to the heme a3/CuB site. The transfer occurs through the D-channel, because it is observed also in the N139D/K362M double mutant in which the K-channel is blocked. It is concluded that the intermediate electrogenic phase observed in the wild type enzyme is missing in the N139D mutant and is because of translocation of the "pumped" proton from Glu-286 to the D-ring propionate of heme a3 or to release of this proton to the outer aqueous phase. Significantly, with the wild type oxidase, the protonic electrogenic phase associated with proton pumping (approximately 0.4 ms) precedes the electrogenic phase associated with the oxygen chemistry (approximately 1.5 ms).     

The role of water in the extracellular half channel of bacteriorhodopsin.

The changes in the photocycle of the wild type and several mutant bacteriorhodopsin (D96N, E204Q, and D212N) were studied on dried samples, at relative humidities of 100% and 50%. Samples were prepared from suspensions at pH approximately 5 and at pH approximately 9. Intermediate M with unprotonated Schiff base was observed at the lower humidity, even in the case where the photocycle in suspension did not contain this intermediate (mutant D212N, high pH). The photocycle of the dried sample stopped at intermediate M1 in the extracellular conformation; conformation change, switching the accessibility of the Schiff base to the cytoplasmic side, and proton transport did not occur. The photocycle decayed slowly by dissipating the absorbed energy of the photon, and the protein returned to its initial bacteriorhodopsin state, through several M1-like substates. These substates presumably reflect different paths of the proton back to the Schiff base, as a consequence of the bacteriorhodopsin adopting different conformations by stiffening on dehydration. All intermediates requiring conformational change were hindered in the dried form. The concentration of intermediate L, which appears after isomerization of the retinal from all-trans to 13-cis, during local relaxation of the protein, was unusually low in dried samples. The lack of intermediates N and O demonstrated that the M state did not undergo a change from the extracellular to the cytoplasmic conformation (M1 to M2 transition), as already indicated by Fourier transform infrared spectroscopy, quasielastic incoherent neutron scattering, and electric signal measurements described in the literature.     

Arginine-82 regulates the pKa of the group responsible for the light-driven proton release in bacteriorhodopsin.

In wild-type bacteriorhodopsin light-induced proton release occurs before uptake at neutral pH. In contrast, in mutants in which R82 is replaced by a neutral residue (as in R82A and R82Q), only a small fraction of the protons is released before proton uptake at neutral pH; the major fraction is released after uptake. In R82Q the relative amounts of the two types of proton release, "early" (preceding proton uptake) and "late" (following proton uptake), are pH dependent. The main conclusions are that 1) R82 is not the normal light-driven proton release group; early proton release can be observed in the R82Q mutant at higher pH values, suggesting that the proton release group has not been eliminated. 2) R82 affects the pKa of the proton release group both in the unphotolyzed state of the pigment and during the photocycle. In the wild type (in 150 mM salt) the pKa of this group decreases from approximately 9.5 in the unphotolyzed pigment to approximately 5.8 in the M intermediate, leading to early proton release at neutral pH. In the R82 mutants the respective values of pKa of the proton release group in the unphotolyzed pigment and in M are approximately 8 and 7.5 in R82Q (in 1 M salt) and approximately 8 and 6.5 in R82K (in 150 mM KCl). Thus in R82Q the pKa of the proton release group does not decrease enough in the photocycle to allow early proton release from this group at neutral pH. 3) Early proton release in R82Q can be detected as a photocurrent signal that is kinetically distinct from those photocurrents that are due to proton movements from the Schiff base to D85 during M formation and from D96 to the Schiff base during the M-->N transition. 4) In R82Q, at neutral pH, proton uptake from the medium occurs during the formation of O. The proton is released during the O-->bacteriorhodopsin transition, probably from D85 because the normal proton release group cannot deprotonate at this pH. 5) The time constant of early proton release is increased from 85 microseconds in the wild type to 1 ms in R82Q (in 150 mM salt). This can be directly attributed to the increase in the pKa of the proton release group and also explains the uncoupling of proton release from M formation. 6) In the E204Q mutant only late proton release is observed at both neutral and alkaline pH, consistent with the idea that E204 is the proton release group. The proton release is concurrent with the O-->bacteriorhodopsin transition, as in R82Q at neutral pH.     

Aspartate-histidine interaction in the retinal schiff base counterion of the light-driven proton pump of Exiguobacterium sibiricum

One of the distinctive features of eubacterial retinal-based proton pumps, proteorhodopsins, xanthorhodopsin, and others, is hydrogen bonding of the key aspartate residue, the counterion to the retinal Schiff base, to a histidine. We describe properties of the recently found eubacterium proton pump from Exiguobacterium sibiricum (named ESR) expressed in Escherichia coli, especially features that depend on Asp-His interaction, the protonation state of the key aspartate, Asp85, and its ability to accept a proton from the Schiff base during the photocycle. Proton pumping by liposomes and E. coli cells containing ESR occurs in a broad pH range above pH 4.5. Large light-induced pH changes indicate that ESR is a potent proton pump. Replacement of His57 with methionine or asparagine strongly affects the pH-dependent properties of ESR. In the H57M mutant, a dramatic decrease in the quantum yield of chromophore fluorescence emission and a 45 nm blue shift of the absorption maximum with an increase in the pH from 5 to 8 indicate deprotonation of the counterion with a pK(a) of 6.3, which is also the pK(a) at which the M intermediate is observed in the photocycle of the protein solubilized in detergent [dodecyl maltoside (DDM)]. This is in contrast with the case for the wild-type protein, for which the same experiments show that the major fraction of Asp85 is deprotonated at pH >3 and that it protonates only at low pH, with a pK(a) of 2.3. The M intermediate in the wild-type photocycle accumulates only at high pH, with an apparent pK(a) of 9, via deprotonation of a residue interacting with Asp85, presumably His57. In liposomes reconstituted with ESR, the pK(a) values for M formation and spectral shifts are 2-3 pH units lower than in DDM. The distinctively different pH dependencies of the protonation of Asp85 and the accumulation of the M intermediate in the wild-type protein versus the H57M mutant indicate that there is strong Asp-His interaction, which substantially lowers the pK(a) of Asp85 by stabilizing its deprotonated state.     

Aspartic acid 85 in bacteriorhodopsin functions both as proton acceptor and negative counterion to the Schiff base.

In bacteriorhodopsin Asp85 has been proposed to function both as a negative counterion to the Schiff base and as proton acceptor in the early stages of the photocycle. To test this proposal further, we have replaced Asp85 by His. The rationale for this replacement is that although His can function as a proton acceptor, it cannot provide a negative charge at residue 85 to serve as a counterion to the protonated Schiff base. We show here that the absorption spectrum of the D85H mutant is highly sensitive to the pH of the external medium. From spectroscopic titrations, we have determined the apparent pK for deprotonation of the Schiff base to be 8.8 +/- 0.1 and the apparent pK for protonation of the His85 side chain to be approximately 3.5. Between pH 3.5 and 8.8, where the Schiff base is protonated, and the His side chain is deprotonated, the D85H mutant is completely inactive in proton transport. Time-resolved studies show that there is no detectable formation of an M-like intermediate in the photocycle of the D85H mutant. These experiments show that the presence of a neutral proton-accepting moiety at residue 85 is not sufficient for carrying out light-driven proton transport. The requirements at residue 85 are therefore for a group that serves both as a negatively charged counterion and as a proton acceptor.     

Distortion of the L-->M transition in the photocycle of the bacteriorhodopsin mutant D96N: a time-resolved step-scan FTIR investigation

The D96N mutant of bacteriorhodopsin has often been taken as a model system to study the M intermediate of the wild type photocycle due to the long life time of the corresponding intermediate of the mutant. Using time-resolved step-scan FTIR spectroscopy in combination with a sample changing wheel we investigated the photocycle of the mutant with microsecond time resolution. Already after several microseconds an intermediate similar to the MN state is observed, which contrasts with the M state of the wild type protein. At reduced hydration M and N intermediates similar to those of wild type BR can be detected. These results have a bearing on the interpretation of the photocycle of this mutant. A mechanism is suggested for the fast rise of MN which provides some insight into the molecular events involved in triggering the opening of the cytosolic channel also of the wild type protein.     

Contribution of proton release to the B2 photocurrent of bacteriorhodopsin.

The contribution of proton release from the so-called proton release group to the microsecond B2 photocurrent from bacteriorhodopsin (bR) oriented in polyacrylamide gels was determined. The fraction of the B2 current due to proton release was resolved by titration of the proton release group in M. At pH values below the pKa of the proton release group in M, the proton release group cannot release its proton during the first half of the bacteriorhodopsin photocycle. At these pH values, the B2 photocurrent is due primarily to translocation of the Schiff base proton to Asp85. The B2 photocurrent was measured in wild-type bR gels at pH 4.5-7.5, in 100 mM KCl/50 mM phosphate. The B2 photocurrent area (proportional to the amount of charge moved) exhibits a pH dependence with a pKa of 6.1. This is suggested to be the pKa of the proton release group in M; the value obtained is in good agreement with previous results obtained by examining photocycle kinetics and pH-sensitive dye signals. In the mutant Glu204Gln, the B2 photocurrent of the mutant membranes was pH independent between pH 4 and 7. Because the proton release group is incapacitated, and early proton release is eliminated in the Glu204Gln mutant, this supports the idea that the pH dependence of the B2 photocurrent in the wild type reflects the titration of the proton release group. In wild-type bacteriorhodopsin, proton release contributes approximately half of the B2 area at pH 7.5. The B2 area in the Glu204Gln mutant is similar to that in the wild type at pH 4.5; in both cases, the B2 current is likely due only to movement of the Schiff base proton to Asp85.     

Protonation reactions and their coupling in bacteriorhodopsin

Light-induced changes of the proton affinities of amino acid side groups are the driving force for proton translocation in bacteriorhodopsin. Recent progress in obtaining structures of bacteriorhodopsin and its intermediates with an increasingly higher resolution, together with functional studies utilizing mutant pigments and spectroscopic methods, have provided important information on the molecular architecture of the proton transfer pathways and the key groups involved in proton transport. In the present paper I consider mechanisms of light-induced proton release and uptake and intramolecular proton transport and mechanisms of modulation of proton affinities of key groups in the framework of these data. Special attention is given to some important aspects that have surfaced recently. These are the coupling of protonation states of groups involved in proton transport, the complex titration of the counterion to the Schiff base and its origin, the role of the transient protonation of buried groups in catalysis of the chromophore's thermal isomerization, and the relationship between proton affinities of the groups and the pH dependencies of the rate constants of the photocycle and proton transfer reactions.     

Infrared study of the L, M, and N intermediates of bacteriorhodopsin using the photoreaction of M.

Infrared spectroscopy is used to characterize the transitions in the photocycle of bR involving the M intermediate. It has been shown previously that in this part of the photocycle a large protein conformational change takes place that is important for proton pumping. In this work we separate the spectra of the L, M, and N intermediates in order to better describe the timing of the molecular changes. We use the photoreaction of the M intermediate to separate its spectrum from those of L and N. At temperatures between 220 and 270 K a mixture of M and L or N is produced by illumination with green light. Subsequent blue illumination selectively drives M back into the ground state and the difference between the spectra before and after blue excitation yields the spectrum of M. Below about 250 K and L/M mixture is separated; at higher temperatures an M/N mixture is seen. We find that the spectrum of M is identical in the two temperature regions. The large protein conformational change is seen to occur during the M to N transition. Our results confirm that Asp-96 is transiently deprotonated in the L state. The only aspartic protonation changes between M and bR are the protonation of Asp-85 and Asp-212 that occur simultaneously during the L to M transition. Blue-light excitation of M results in deprotonation of both. The results suggest a quadrupolelike interaction of the Schiff base, Asp-85, Asp-212, and an additional positive charge in bR.     

Charge transfer in green fluorescent protein.

Charge transfer reactions that contribute to the photoreactions of the wild type green fluorescent protein (GFP) do not occur in the isolated p-hydroxybenzylidene-imidazolidinone chromophore, demonstrating the role of the protein environment. The high quantum efficiency of the fluorescence photocycle that includes excited state proton transfer and the suppression of non-radiative pathways by the protein environment have been correlated with structural dynamics in the chromophore environment. A low quantum efficiency competing phototransformation reaction of GFP is accompanied by both proton and electron transfer, and closely mimics the charge redistribution that is occurring in the fluorescence photocycle. The protein response to this destabilising event has been demonstrated by cryo-trapping of early products in the reaction pathway and is found to be strong even at 100 K, including displacements of chromophore, protein, solvent and a photogenerated CO2 molecule derived from the decarboxylated Glu 222 side chain. We discuss the ramifications of the observation of strong conformational perturbations below the protein dynamical transition at approximately 200 K, in view of low temperature work on other light sensitive proteins such as myoglobin and bacteriorhodopsin. The proton and electron transfer in the phototransformation pathway mimics the proton and charge transfer which occurs during the fluorescence cycle, which leads to common structural responses in both photoreactions as shown by ultrafast spectroscopy. We review and discuss literature on light-induced and thermal charge transfer events, focusing on recent findings addressing conformational dynamics and implications for thermodynamic properties.     

His166 is critical for active-site proton transfer and phototaxis signaling by sensory rhodopsin I.

Photoinduced deprotonation of the retinylidene Schiff base in the sensory rhodopsin I transducer (SRI-Htrl) complex results in formation of the phototaxis signaling state S373. Here we report identification of a residue, His166, critical to this process, as well as to reprotonation of the Schiff base during the recovery phase of the SRI photocycle. Each of the residue substitutions A, D, G, L, S, V, or Y at position 166 reduces the flash yield of S373, to values ranging from 2% of wild type for H166Y to 23% for H166V. The yield of S373 is restored to wild-type levels in Htrl-free H166L by alkaline deprotonation of Asp76, a Schiff base proton acceptor normally not ionized in the SRI-Htrl complex, showing that proton transfer from the Schiff base in H166L occurs when an acceptor is made available. The flash yield and rate of decay of S373 of the mutants are pH dependent, even when complexed with Htrl, which confers pH insensitivity to wild-type SRI, suggesting that partial disruption of the complex has occurred. The rates of S373 reprotonation at neutral pH are also prolonged in all H166X mutants, with half-times from 5 s to 160 s (wild type, 1 s). All mutations of His166 tested disrupt phototaxis signaling. No response (H166D, H166L), dramatically reduced responses (H166V), or inverted responses to orange light (H166A, H166G, H166S, and H166Y) or to both orange and near-UV light (H166Y) are observed. Our conclusions are that His166 1) plays a role in the pathways of proton transfer both to and from the Schiff base in the SRI-Htrl complex, either as a structurally important residue or possibly as a participant in proton transfers; 2) is involved in the modulation of SRI photoreaction kinetics by Htrl; and 3) is important in phototaxis signaling. Consistent with the involvement of the His imidazole moiety, the addition of 10 mM imidazole to membrane suspensions containing H166A receptors accelerates S373 decay 10-fold at neutral pH, and a negligible effect is seen on wild-type SRI.     

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

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

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.     

Fourier transform infrared evidence for Schiff base alteration in the first step of the bacteriorhodopsin photocycle

The first step of the bacteriorhodopsin (bR) photocycle involves the formation of a red-shifted product, K. Fourier transform infrared difference spectra of the bR570 to K630 transition at 81 K has been measured for bR containing different isotopic substitutions at the retinal Schiff base. In the case of bacteriorhodopsin containing a deuterium substitution at the Schiff base nitrogen, carbon 15, or both, we find spectral changes in the 1600-1610- and 1570-1580-cm-1 region consistent with the hypothesis that the K630 C=N stretching mode of a protonated Schiff base is located near 1609 cm-1. A similar set of Schiff base deuterium substitutions for retinal containing a 13C at the carbon 10 position strongly supports this conclusion. This assignment of the K630 C=N stretching vibration provides evidence that the bR Schiff base proton undergoes a substantial environmental change most likely due to separation from a counterion. In addition, a correlation is found between the C=N stretching frequency and the maximum wavelength of visible absorption, suggesting that movement of a counterion relative to the Schiff base proton is the main source of absorption changes in the early stages of the photocycle. Such a movement is a key prediction of several models of proton transport and energy transduction. Evidence is also presented that one or more COOH groups are involved in the formation of the K intermediate.     

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.     

Monitoring light-induced structural changes of Channelrhodopsin-2 by UV-visible and Fourier transform infrared spectroscopy

Channelrhodopsin-2 (ChR2) is a microbial type rhodopsin and a light-gated cation channel that controls phototaxis in Chlamydomonas. We expressed ChR2 in COS-cells, purified it, and subsequently investigated this unusual photoreceptor by flash photolysis and UV-visible and Fourier transform infrared difference spectroscopy. Several transient photoproducts of the wild type ChR2 were identified, and their kinetics and molecular properties were compared with those of the ChR2 mutant E90Q. Based on the spectroscopic data we developed a model of the photocycle comprising six distinguishable intermediates. This photocycle shows similarities to the photocycle of the ChR2-related Channelrhodopsin of Volvox but also displays significant differences. We show that molecular changes include retinal isomerization, changes in hydrogen bonding of carboxylic acids, and large alterations of the protein backbone structure. These alterations are stronger than those observed in the photocycle of other microbial rhodopsins like bacteriorhodopsin and are related to those occurring in animal rhodopsins. UV-visible and Fourier transform infrared difference spectroscopy revealed two late intermediates with different time constants of tau = 6 and 40 s that exist during the recovery of the dark state. The carboxylic side chain of Glu(90) is involved in the slow transition. The molecular changes during the ChR2 photocycle are discussed with respect to other members of the rhodopsin family.     

Evidence for long range allosteric interactions between the extracellular and cytoplasmic parts of bacteriorhodopsin from the mutant R82A and its second site revertant R82A/G231C

Evidence is presented for long range interactions between the extracellular and cytoplasmic parts of the heptahelical membrane protein bacteriorhodopsin in the mutant R82A and its second site revertant R82A/G231C. (i) In the double mutants R82A/G72C and R82A/A160C, with the cysteine mutation on the extracellular or cytoplasmic surface, respectively, the photocycle is the same as in the single mutant R82A with an accelerated deprotonation of the Schiff base and a reversed order of proton release and uptake. Proton release and uptake kinetics were measured directly at either surface by using the unique cysteine residue as attachment site for the pH indicator fluorescein. Whereas in wild type proton uptake on the cytoplasmic surface occurs during the M-decay (tau approximately 8 ms), in R82A it occurs already during the first phase of the M-rise (tau < 1 microseconds). (ii) The introduction of a second mutation at the cytoplasmic surface in position 231 (helix G) restores wild type ground state absorption properties, kinetics of photocycle and of proton release, and uptake in the mutant R82A/G231C. In addition, kinetic H/D isotope effects provide evidence that the proton release mechanism in R82A/G231C and in wild type is similar. These results suggest the existence of long range interactions between the cytoplasmic and extracellular surface domains of bacteriorhodopsin mediated by salt bridges and hydrogen-bonded networks between helices C (Arg-82) and G (Asp-212 and Gly-231). Such long range interactions are expected to be of functional significance for activation and signal transduction in heptahelical G-protein-coupled receptors.     

Photocycle in the M-form in bacteriorhodopsin mutants devoid of primary proton acceptor Asp-85

Photoinduced changes in absorption of the deprotonated M-form in the mutant bacteriorhodopsin without primary proton acceptor Asp-85 were studied and additional evidence in support of the complete transmembrane proton transfer in photocycle was obtained. Measurements of the absorption spectrum were carried out at various pH, temperature, and humidity. The direction of proton transfer was the same as in the normal photocycle of the wild-type bacteriorhodopsin: from the internal to the external side of the membrane. The effect on this process of a terminal acceptor Glu-204 was shown.