The role of Glu181 in the photoactivation of rhodopsin

The visual pigment rhodopsin is a prototypical seven transmembrane helical G protein-coupled receptor. Photoisomerization of its protonated Schiff base (PSB) retinylidene chromophore initiates a progression of metastable intermediates. We studied the structural dynamics of receptor activation by FTIR spectroscopy of recombinant pigments. Formation of the active state, Meta II, is characterized by neutralization of the PSB and its counterion Glu113. We focused on testing the hypothesis of a PSB counterion switch from Glu113 to Glu181 during the transition of rhodopsin to the still inactive Meta I photointermediate. Our results, especially from studies of the E181Q mutant, support the view that both Glu113 and Glu181 are deprotonated, forming a complex counterion to the PSB in rhodopsin, and that the function of the primary counterion shifts from Glu113 to Glu181 during the transition to Meta I. The Meta I conformation in the E181Q mutant is less constrained compared with that of wild-type Meta I. In particular, the hydrogen bonded network linking transmembrane helices 1, 2, and 7, adopts a conformation that is already Meta II-like, while other parts of the receptor appear to be in a Meta I-like conformation similar to wild-type. We conclude that Glu181 is responsible, in part, for controlling the extraordinary high pK(a) of the chromophore PSB in the dark state, which very likely decreases upon transition to Meta I in a stepwise weakening of the interaction between PSB and its complex counterion during the course of receptor activation. A model for the specific role in coupling chromophore isomerization to protein conformational changes concomitant with receptor activation is presented.     

Structural impact of the E113Q counterion mutation on the activation and deactivation pathways of the G protein-coupled receptor rhodopsin

Disruption of an interhelical salt bridge between the retinal protonated Schiff base linked to H7 and Glu113 on H3 is one of the decisive steps during activation of rhodopsin. Using previously established stabilization strategies, we engineered a stabilized E113Q counterion mutant that converted rhodopsin to a UV-absorbing photoreceptor with deprotonated Schiff base and allowed reconstitution into native-like lipid membranes. Fourier-transform infrared difference spectroscopy reveals a deprotonated Schiff base in the photoproducts of the mutant up to the active state Meta II, the absence of the classical pH-dependent Meta I/Meta II conformational equilibrium in favor of Meta II, and an anticipation of active state features under conditions that stabilize inactive photoproduct states in wildtype rhodopsin. Glu181 on extracellular loop 2, is found to be unable to maintain a counterion function to the Schiff base on the activation pathway of rhodopsin in the absence of the primary counterion, Glu113. The Schiff base becomes protonated in the transition to Meta III. This protonation is, however, not associated with a deactivation of the receptor, in contrast to wildtype rhodopsin. Glu181 is suggested to be the counterion in the Meta III state of the mutant and appears to be capable of stabilizing a protonated Schiff base in Meta III, but not of constraining the receptor in an inactive conformation.     

Changing the location of the Schiff base counterion in rhodopsin.

Rhodopsin and all of the vertebrate visual pigments have a carboxylic acid residue, Glu113, in the third transmembrane segment that serves as a counterion to the protonated Schiff base nitrogen of the chromophore. We show here that the counterion in bovine rhodopsin can be moved from position 113 to 117 without significantly changing the wild-type spectral properties of the protein. A series of double mutants were constructed where the Glu113 counterion was changed to Gln and an Asp residue was substituted for amino acid residues from position 111 to 121 in the third transmembrane segment of the protein. Only at position 117 can an Asp fully substitute for the counterion at position 113. The double mutant E113Q,-A117D has an absorption maximum at 493 nm which is independent of pH in the range 5.6-8.4 and independent of the presence of external chloride anions. An Asp at no other position tested in the third transmembrane segment can fully substitute for the Glu counterion at position 113. Partial substitution is observed for an Asp at position 120. Residues 113, 117, and 120 are expected to lie along the same face of an alpha-helix. These results suggest that the Schiff base nitrogen in rhodopsin is located between residues 113 and 117 but there is enough flexibility in the protein to allow partial interaction with an Asp at position 120. Position 117 is the same location of the counterion in the related biogenic amine receptors.     

Structural changes of water molecules during the photoactivation processes in bovine rhodopsin

Internal water molecules of rhodopsins play an important role in stabilizing the crucial ion pair comprised by the protonated retinal Schiff base and its counterion. Previous low-temperature FTIR spectroscopy of archaeal rhodopsins observed water O-D stretching vibrations at 2400-2100 cm(-1) in D(2)O, corresponding to strong hydrogen bonds. Since a water molecule bridges the protonated Schiff base and an aspartate in archaeal rhodopsins, the observed water molecules presumably hydrate the negative charges in the Schiff base region. In contrast, the FTIR spectroscopy data of bovine rhodopsin presented here revealed that there are no spectral changes of water molecules under strongly hydrogen-bonding conditions (in the range <2400 cm(-1) for O-D stretch) during the photoactivation processes. The only observed water bands were located in the >2500 cm(-1) region that corresponds to weak hydrogen bonding. These results imply that the ion pair state in vertebrate visual rhodopsins is stabilized in a manner different from that in archaeal rhodopsins. In addition, the internal water molecules that hydrate the negative charges do not play important role in the photoactivation processes of rhodopsin that involve proton transfer from the Schiff base to Glu113 upon formation of Meta II. Structural changes of the H-D exchangeable peptide amide of a beta-sheet are observed upon formation of metarhodopsin II, suggesting that motion of a beta-sheet is coupled to the proton transfer reaction from the Schiff base to its counterion.     

Constitutive activity of a UV cone opsin

Vertebrate visual pigment proteins contain a conserved carboxylic acid residue in the third transmembrane helix. In rhodopsin, Glu113 serves as a counterion to the positively charged protonated Schiff base formed by 11-cis retinal attached to Lys296. Activation involves breaking of this ion pair. In UV cone pigments, the retinyl Schiff base is unprotonated, and hence such a salt bridge is not present; yet the pigment is inactive in the dark. Mutation of Glu108, which corresponds to rhodopsin's Glu113, to Gln yields a pigment that remains inactive in the dark. The apoproteins of both the wild-type and mutant, however, are constitutively active with the mutant being of significantly higher activity. Thus, one important role for preserving the negatively charged glutamate in the third helix of UV pigments is to maintain a less active opsin in a manner similar to rhodopsin. Ligand binding itself in the absence of a salt bridge is sufficient for deactivation.     

pH dependence of photolysis intermediates in the photoactivation of rhodopsin mutant E113Q

Glutamic acid at position 113 in bovine rhodopsin ionizes to form the counterion to the protonated Schiff base (PSB), which links the 11-cis-retinylidene chromophore to opsin. Photoactivation of rhodopsin requires both Schiff base deprotonation and neutralization of Glu-113. To better understand the role of electrostatic interactions in receptor photoactivation, absorbance difference spectra were collected at time delays from 30 ns to 690 ms after photolysis of rhodopsin mutant E113Q solubilized in dodecyl maltoside at different pH values at 20 degrees C. The PSB form (pH 5. 5, lambda(max) = 496 nm) and the unprotonated Schiff base form (pH 8. 2, lambda(max) = 384 nm) of E113Q rhodopsin were excited using 477 nm or 355 nm light, respectively. Early photointermediates of both forms of E113Q were qualitatively similar to those of wild-type rhodopsin. In particular, early photoproducts with spectral shifts to longer wavelengths analogous to wild-type bathorhodopsin were seen. In the case of the basic form of E113Q, the absorption maximum of this intermediate was at 408 nm. These results suggest that steric interaction between the retinylidene chromophore and opsin, rather than charge separation, plays the dominant role in energy storage in bathorhodopsin. After lumirhodopsin, instead of deprotonating to form metarhodopsin I(380) on the submillisecond time scale as is the case for wild type, the acidic form of E113Q produced metarhodopsin I(480), which decayed very slowly (exponential lifetime = 12 ms). These results show that Glu-113 must be present for efficient deprotonation of the Schiff base and rapid visual transduction in vertebrate visual pigments.     

Resonance Raman microprobe spectroscopy of rhodopsin mutants: effect of substitutions in the third transmembrane helix.

A microprobe system has been developed that can record Raman spectra from as little as 2 microL of solution containing only micrograms of biological pigments. The apparatus consists of a liquid nitrogen (l-N2)-cooled cold stage, an epi-illumination microscope, and a substractive-dispersion, double spectrograph coupled to a l-N2-cooled CCD detector. Experiments were performed on native bovine rhodopsin, rhodopsin expressed in COS cells, and four rhodopsin mutants: Glu134 replaced by Gln (E134Q), Glu122 replaced by Gln (E122Q), and Glu113 replaced by Gln (E113Q) or Ala (E113A). Resonance Raman spectra of photostationary steady-state mixtures of 11-cis-rhodopsin, 9-cis-isorhodopsin, and all-trans-bathorhodopsin at 77 K were recorded. The Raman spectra of E134Q and the wild-type are the same, indicating that Glu134 is not located near the chromophore. Substitution at Glu122 also does not affect the C = NH stretching vibration of the chromophore. The fingerprint and Schiff base regions of the Raman spectra of the 380-nm, pH 7 forms of E113Q and E113A are characteristic of unprotonated retinal Schiff bases. The C = NH modes of the approximately 500-nm, pH 5 forms of E113Q and E113A in H2O (D2O) are found at 1648 (1629) and 1645 (1630) cm-1, respectively. These frequencies indicate that the protonated Schiff base interacts more weakly with its protein counterion in the Glu113 mutants than it does in the native pigment. Furthermore, perturbations of the unique bathorhodopsin hydrogen out-of-plane (HOOP) vibrations in E113Q and E113A indicate that the strength of the protein perturbation near C12 is weakened compared to that in native bathorhodopsin.(ABSTRACT TRUNCATED AT 250 WORDS)     

Constitutively active mutants of rhodopsin.

Two critical amino acids in the visual pigment rhodopsin are Lys-296, the site of attachment of retinal to the protein through a protonated Schiff base linkage, and Glu-113, the Schiff base counterion. Mutation of Lys-296 or Glu-113 results in constitutive activation of opsin, as assayed by its ability to activate transducin in the absence of added chromophore. We conclude that opsin is constrained to an inactive conformation by a salt bridge between Lys-296 and Glu-113. Recently, one of the mutants, K296E, was found in a family with retinitis pigmentosa, suggesting that degeneration of the photoreceptor cells in individuals with this mutation may result from persistent stimulation of the phototransduction pathway.     

Characterization of rhodopsin congenital night blindness mutant T94I

The Thr94 --> Ile mutation in the second transmembrane segment of rhodopsin has been reported to be associated with a congenital night blindness phenotype in a large Irish pedigree. Previously, two other known rhodopsin mutants that cause congenital night blindness, A292E and G90D, have been shown in vitro to constitutively activate the G protein transducin in the absence of a chromophore. The proposed mechanism of constitutive activation of these two mutants is an electrostatic disruption of the active site salt bridge between Glu113 and Lys296 that contributes to stabilization of the protein in the inactive state. Here, the T94I rhodopsin mutant is characterized and compared to the two other known rhodopsin night blindness mutants. The T94I mutant opsin is shown also to constitutively activate transducin. The T94I mutant pigment (with a bound 11-cis-retinal chromophore), like the other known rhodopsin night blindness mutants, is not active in the dark and has wild-type activity upon exposure to light. Similar to the Gly90 --> Asp substitution, position 94 is close enough to the Schiff base nitrogen that an Asp at this position can functionally substitute for the Glu113 counterion. However, in contrast to the other night blindness mutants, the T94I MII intermediate decays with a half-life that is approximately 8-fold slower than in the wild-type MII intermediate. Thus, the one phenotype shared by all congenital night blindness mutants that is different from the wild-type protein is constitutive activation of the apoprotein.     

Retinal isomerization in bacteriorhodopsin is controlled by specific chromophore-protein interactions. A study with noncovalent artificial pigments.

It has previously been shown that, in mutants lacking the Lys-216 residue, protonated Schiff bases of retinal occupy noncovalently the bacteriorhodopsin (bR) binding site. Moreover, the retinal-Lys-216 covalent bond is not a prerequisite for initiating the photochemical and proton pump activity of the pigment. In the present work, various Schiff bases of aromatic polyene chromophores were incubated with bacterioopsin to give noncovalent pigments that retain the Lys-216 residue in the binding site. It was observed that the pigment's absorption was considerably red-shifted relative to the corresponding protonated Schiff bases (PSB) in solution and was sensitive to Schiff base linkage substitution. Their PSB pK(a) is considerably elevated, similarly to those of related covalently bound pigments. However, the characteristic low-pH purple to blue transition is not observed, but rather a chromophore release from the binding site takes place that is characterized by a pK(a) of approximately 6 (sensitive to the specific complex). It is suggested that, in variance with native bR, in these complexes Asp-85 is protonated and Asp-212 serves as the sole negatively charged counterion. In contrast to the bound analogues, no photocycle could be detected. It is suggested that a specific retinal-protein geometrical arrangement in the binding site is a prerequisite for achieving the selective retinal photoisomerization.     

Slow binding of retinal to rhodopsin mutants G90D and T94D

In an examination of the effect of three rhodopsin night blindness mutations on the rate of association of 11-cis-retinal with opsin, one of the mutations (G90D) was found to slow the rate of reaction by more than 80-fold. This effect does not appear to be general to night blindness mutations as the two other mutants (A292E and T94I) were not found to bind retinal with slowed kinetics. However, T94D was similar to G90D in that the rate of retinal binding was dramatically slowed. Gly90 and Thr94 are both located in the active site of the protein close to the Schiff base counterion Glu113. Thus, the slow kinetics of Schiff base formation appear to correlate with the introduction of a negative charge close to the Schiff base counterion, suggesting a possible role for Glu113 as a catalytic base in this reaction. Consistent with this model, the E113Q mutant was also found to bind retinal more slowly than the wild type.     

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.     

Solid state 15N NMR evidence for a complex Schiff base counterion in the visual G-protein-coupled receptor rhodopsin.

Using the baculovirus/Sf9 cell expression system, we have incorporated 99% 15N-enriched [alpha,epsilon-15N2]-L-lysine into the rod visual pigment rhodopsin. We have subsequently investigated the protonated Schiff base (pSB) linkage in the [alpha, epsilon-15N2]Lys-rhodopsin with cross-polarization magic angle spinning (CP/MAS) 15N NMR. The Schiff base (SB) 15N in [alpha, epsilon-15N2]Lys-rhodopsin resonates with an isotropic shift sigmaI of 155.9 ppm, relative to 5.6 M 15NH4Cl. This suggests that the SB in rhodopsin is protonated and stabilized by a complex counterion. The 15N shifts of retinal SBs correlate with the energy difference between the ground and excited states and the frequency of maximum visible absorbance, numax, associated with the pi-pi transition of the polyene chromophore. Experimental modeling of the relation between the numax and the size of the counterion with a set of pSBs provides strong evidence that the charged chromophore in rhodopsin is stabilized by a counterion with an estimated effective center-center distance (deff) between the counterion and the pSB of 0.43 +/- 0.01 nm. While selected prokaryotic proteins and complexes have been labeled before, this is the first time to our knowledge that a 15N-labeled eukaryotic membrane protein has been generated in sufficient amount for such NMR investigations.     

A study of the Schiff base mode in bovine rhodopsin and bathorhodopsin

We have obtained the resonance Raman spectra of bovine rhodopsin, bathorhodopsin, and isorhodopsin for a series of isotopically labeled retinal chromophores. The specific substitutions are at retinal's protonated Schiff base moiety and include -HC = NH+-, -HC = ND+-, -H13C = NH+-, and -H13C = ND+-. Apart from the doubly labeled retinal, we find that the protonated Schiff base frequency is the same, within experimental error, for both rhodopsin and bathorhodopsin for all the substitutions measured here and elsewhere. We develop a force field that accurately fits the observed ethylenic (C = C) and protonated Schiff base stretching frequencies of rhodopsin and labeled derivatives. Using MINDO/3 quantum mechanical procedures, we investigate the response of this force field, and the ethylenic and Schiff base stretching frequencies, to the placement of charges close to retinal's Schiff base moiety. Specifically, we find that the Schiff base frequency should be measurably affected by a 3.0-4.5-A movement of a negatively charged counterion from the positively charged protonated Schiff base moiety. That there is no experimentally discernible difference in the Schiff base frequency between rhodopsin and bathorhodopsin suggests that models for the efficient conversion of light to chemical energy in the rhodopsin to bathorhodopsin photoconversion based solely on salt bridge separation of the protonated Schiff base and its counterion are probably incorrect. We discuss various alternative models and the role of electrostatics in the rhodopsin to bathorhodopsin primary process.     

A large photolysis-induced pKa increase of the chromophore counterion in bacteriorhodopsin: implications for ion transport mechanisms of retinal proteins.

The proton-pumping mechanism of bacteriorhodopsin is dependent on a photolysis-induced transfer of a proton from the retinylidene Schiff base chromophore to the aspartate-85 counterion. Up until now, this transfer was ascribed to a > 7-unit decrease in the pKa of the protonated Schiff base caused by photoisomerization of the retinal. However, a comparably large increase in the pKa of the Asp-85 acceptor also plays a role, as we show here with infrared measurements. Furthermore, the shifted vibrational frequency of the Asp-85 COOH group indicates a transient drop in the effective dielectric constant around Asp-85 to approximately 2 in the M photointermediate. This dielectric decrease would cause a > 40 kJ-mol-1 increase in free energy of the anionic form of Asp-85, fully explaining the observed pK alpha increase. An analogous photolysis-induced destabilization of the Schiff base counterion could initiate anion transport in the related protein, halorhodopsin, in which aspartate-85 is replaced by Cl- and the Schiff base proton is consequently never transferred.     

Photoisomerization efficiency in UV-absorbing visual pigments: protein-directed isomerization of an unprotonated retinal Schiff base

A visual pigment consists of an opsin protein and a chromophore, 11-cis-retinal, which binds to a specific lysine residue of opsin via a Schiff base linkage. The Schiff base chromophore is protonated in pigments that absorb visible light, whereas it is unprotonated in ultraviolet-absorbing visual pigments (UV pigments). To investigate whether an unprotonated Schiff base can undergo photoisomerization as efficiently as a protonated Schiff base in the opsin environment, we measured the quantum yields of the bovine rhodopsin E113Q mutant, in which the Schiff base is unprotonated at alkaline pH, and the mouse UV pigment (mouse UV). Photosensitivities of UV pigments were measured by irradiation of the pigments followed by chromophore extraction and HPLC analysis. Extinction coefficients were estimated by comparing the maximum absorbances of the original pigments and their acid-denatured states. The quantum yield of the bovine rhodopsin E113Q mutant at pH 8.2, where the Schiff base is unprotonated, was significantly lower than that of wild-type rhodopsin, whereas the mutant gave a quantum yield almost identical to that of the wild type at pH 5.5, where the Schiff base is protonated. These results suggest that Schiff base protonation plays a role in increasing quantum yield. The quantum yield of mouse UV, which has an unprotonated Schiff base chromophore, was significantly higher than that of the unprotonated form of the rhodopsin E113Q mutant, although it was still lower than the visible-absorbing pigments. These results suggest that the mouse UV pigment has a specific mechanism for the efficient photoisomerization of its unprotonated Schiff base chromophore.     

Role of the retinal hydrogen bond network in rhodopsin Schiff base stability and hydrolysis

Little is known about the molecular mechanism of Schiff base hydrolysis in rhodopsin. We report here our investigation into this process focusing on the role of amino acids involved in a hydrogen bond network around the retinal Schiff base. We find conservative mutations in this network (T94I, E113Q, S186A, E181Q, Y192F, and Y268F) increase the activation energy (E(a)) and abolish the concave Arrhenius plot normally seen for Schiff base hydrolysis in dark state rhodopsin. Interestingly, two mutants (T94I and E113Q) show dramatically faster rates of Schiff base hydrolysis in dark state rhodopsin, yet slower hydrolysis rates in the active MII form. We find deuterium affects the hydrolysis process in wild-type rhodopsin, exhibiting a specific isotope effect of approximately 2.5, and proton inventory studies indicate that multiple proton transfer events occur during the process of Schiff base hydrolysis for both dark state and MII forms. Taken together, our study demonstrates the importance of the retinal hydrogen bond network both in maintaining Schiff base integrity in dark state rhodopsin, as well as in catalyzing the hydrolysis and release of retinal from the MII form. Finally, we note that the dramatic alteration of Schiff base stability caused by mutation T94I may play a causative role in congenital night blindness as has been suggested by the Oprian and Garriga laboratories.     

Chromophore structure in lumirhodopsin and metarhodopsin I by time-resolved resonance Raman microchip spectroscopy.

Time-resolved resonance Raman microchip flow experiments have been performed on the lumirhodopsin (Lumi) and metarhodopsin I (Meta I) photointermediates of rhodopsin at room temperature to elucidate the structure of the chromophore in each species as well as changes in protein-chromophore interactions. Transient Raman spectra of Lumi and Meta I with delay times of 16 micros and 1 ms, respectively, are obtained by using a microprobe system to focus displaced pump and probe laser beams in a microfabricated flow channel and to detect the scattering. The fingerprint modes of both species are very similar and characteristic of an all-trans chromophore. Lumi exhibits a relatively normal hydrogen-out-of-plane (HOOP) doublet at 951/959 cm(-1), while Meta I has a single HOOP band at 957 cm(-1). These results suggest that the transitions from bathorhodopsin to Lumi and Meta I involve a relaxation of the chromophore to a more planar all-trans conformation and the elimination of the structural perturbation that uncouples the 11H and 12H wags in bathorhodopsin. Surprisingly, the protonated Schiff base C=N stretching mode in Lumi (1638 cm(-1)) is unusually low compared to those in rhodopsin and bathorhodopsin, and the C=ND stretching mode shifts down by only 7 cm(-1) in D2O buffer. This indicates that the Schiff base hydrogen bonding is dramatically weakened in the bathorhodopsin to Lumi transition. However, the C=N stretching mode in Meta I is found at 1654 cm(-1) and exhibits a normal deuteration-induced downshift of 24 cm(-1), identical to that of the all-trans protonated Schiff base. The structural relaxation of the chromophore-protein complex in the bathorhodopsin to Lumi transition thus appears to drive the Schiff base group out of its hydrogen-bonded environment near Glu113, and the hydrogen bonding recovers to a normal solvated PSB value but presumably a different hydrogen bond acceptor with the formation of Meta I.     

Mechanism of isomerization of rhodopsin studied by use of 11-cis-locked rhodopsin analogues excited with a picosecond laser pulse

Primary photochemical behaviors of cattle rhodopsin analogues (Rh5 and Rh7) having cyclopenta- and cycloheptatrienylidene 11-cis-locked retinals (Ret5 and Ret7, respectively) were studied by excitation with a picosecond laser pulse (wavelength 532 nm; duration 21 ps). Picosecond absorption and fluorescence measurements of Rh5 showed formation of only a long-lived excited singlet state (tau l/e = 85 ps). The excited state of the retinal analogue having a five-membered ring was stabilized in protein (Rh5) more than in solvent (protonated Schiff base of Ret5; PSB5). Excitation of Rh7 produced two ground-state photoproducts, Rh7 (580) and Rh7 (630). According to the analysis of photon density dependency, Rh7 (580) was a single-photon product of Rh7, while Rh7 (630) was the photoproduct of Rh7 (580). Fluorescence emitted from a seven-membered ring system like Rh7 or a protonated Schiff base of Ret7 (PSB7) was weaker than that in a corresponding five-membered ring system, especially in protein (Rh7). The difference in photoreaction between Rh5 and Rh7 may originate from the difference in fixation of the 11-cis form. On the basis of the spectral and kinetic similarities between Rh7 (580) and photorhodopsin, a precursor of bathorhodopsin, it was proposed that both have twisted all-trans chromophores in the way of the isomerization. The protein moiety of rhodopsin which fixes the chromophore at both ends seems to accelerate the rotation of the C11-C12 double bond and to prevent it from going through relaxation processes other than the isomerization. This may be a plausible reason why rhodopsin has a large quantum yield (0.67).     

Structure of bovine rhodopsin in a trigonal crystal form

We have determined the structure of bovine rhodopsin at 2.65 A resolution using untwinned native crystals in the space group P3(1), by molecular replacement from the 2.8 A model (1F88) solved in space group P4(1). The new structure reveals mechanistically important details unresolved previously, which are considered in the membrane context by docking the structure into a cryo-electron microscopy map of 2D crystals. Kinks in the transmembrane helices facilitate inter-helical polar interactions. Ordered water molecules extend the hydrogen bonding networks, linking Trp265 in the retinal binding pocket to the NPxxY motif near the cytoplasmic boundary, and the Glu113 counterion for the protonated Schiff base to the extracellular surface. Glu113 forms a complex with a water molecule hydrogen bonded between its main chain and side-chain oxygen atoms. This can be expected to stabilise the salt-bridge with the protonated Schiff base linking the 11-cis-retinal to Lys296. The cytoplasmic ends of helices H5 and H6 have been extended by one turn. The G-protein interaction sites mapped to the cytoplasmic ends of H5 and H6 and a spiral extension of H5 are elevated above the bilayer. There is a surface cavity next to the conserved Glu134-Arg135 ion pair. The cytoplasmic loops have the highest temperature factors in the structure, indicative of their flexibility when not interacting with G protein or regulatory proteins. An ordered detergent molecule is seen wrapped around the kink in H6, stabilising the structure around the potential hinge in H6. These findings provide further explanation for the stability of the dark state structure. They support a mechanism for the activation, initiated by photo-isomerisation of the chromophore to its all-trans form, that involves pivoting movements of kinked helices, which, while maintaining hydrophobic contacts in the membrane interior, can be coupled to amplified translation of the helix ends near the membrane surfaces.