Agonists and partial agonists of rhodopsin: retinals with ring modifications

Activation of the visual pigment rhodopsin is initiated by isomerization of its retinal chromophore to the all-trans geometry, which drives the conformation of the protein to the active state. We have examined by FTIR spectroscopy the impact of a series of modifications at the ring of retinal on the activation process and on molecular interactions within the binding pocket. Deletion of ring methyl groups at C1 and C5 or replacement of the ring in diethyl or ethyl-methyl acyclic analogues resulted in partial agonists, for which the conformational equilibrium between the Meta I and Meta II photoproduct is shifted from the active Meta II side to the inactive Meta I side. While the Meta II states of these artificial pigments had a conformation similar to those of native Meta II, the Meta I states were different. Modifications on the ring of retinal had a particular impact on the interaction of Glu 122 within the ring-binding pocket and are shown to interfere with the Glu 134-mediated proton uptake during formation of Meta II. We further found, upon partial deletion of ring constituents, a decrease of the entropy change of the transition from Meta I to Meta II by up to 50%, while the concomitant reduction of the enthalpy term was less pronounced. These findings underline the particular importance of the ring and the ring methyl groups and are discussed in a model of receptor activation.     

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.     

Functional role of the "ionic lock"--an interhelical hydrogen-bond network in family A heptahelical receptors

Activation of family A G-protein-coupled receptors involves a rearrangement of a conserved interhelical cytoplasmic hydrogen bond network between the E(D)RY motif on transmembrane helix 3 (H3) and residues on H6, which is commonly termed the cytoplasmic “ionic lock.” Glu134^3.49 of the E(D)RY motif also forms an intrahelical salt bridge with neighboring Arg135^3.50 in the dark-state crystal structure of rhodopsin. We examined the roles of Glu134^3.49 and Arg135^3.50 on H3 and Glu247^6.30 and Glu249^6.32 on H6 on the activation of rhodopsin using Fourier transform infrared spectroscopy of wild-type and mutant pigments reconstituted into lipid membranes. Activation of rhodopsin is pH-dependent with proton uptake during the transition from the inactive Meta I to the active Meta II state. Glu134^3.49 of the ERY motif is identified as the proton-accepting group, using the Fourier transform infrared protonation signature and the absence of a pH dependence of activation in the E134Q mutant. Neutralization of Arg135^3.50 similarly leads to pH-independent receptor activation, but with structural alterations in the Meta II state. Neutralization of Glu247^6.30 and Glu249^6.32 on H6, which are involved in interhelical interactions with H3 and H7, respectively, led to a shift toward Meta II in the E247Q and E249Q mutants while retaining the pH sensitivity of the equilibrium. Disruption of the interhelical interaction of Glu247^6.30 and Glu249^6.32 on H6 with H3 and H7 plays its role during receptor activation, but neutralization of the intrahelical salt bridge between Glu134^3.49 and Arg135^3.50 is considerably more critical for shifting the photoproduct equilibrium to the active conformation. These conclusions are discussed in the context of recent structural data of the β₂-adrenergic receptor.     

The 9-methyl group of retinal is essential for rapid Meta II decay and phototransduction quenching in red cones

Cone photoreceptors of the vertebrate retina terminate their response to light much faster than rod photoreceptors. However, the molecular mechanisms underlying this rapid response termination in cones are poorly understood. The experiments presented here tested two related hypotheses: first, that the rapid decay rate of metarhodopsin (Meta) II in red-sensitive cones depends on interactions between the 9-methyl group of retinal and the opsin part of the pigment molecule, and second, that rapid Meta II decay is critical for rapid recovery from saturation of red-sensitive cones after exposure to bright light. Microspectrophotometric measurements of pigment photolysis, microfluorometric measurements of retinol production, and single-cell electrophysiological recordings of flash responses of salamander cones were performed to test these hypotheses. In all cases, cones were bleached and their visual pigment was regenerated with either 11-cis retinal or with 11-cis 9-demethyl retinal, an analogue of retinal lacking the 9-methyl group. Meta II decay was four to five times slower and subsequent retinol production was three to four times slower in red-sensitive cones lacking the 9-methyl group of retinal. This was accompanied by a significant slowing of the recovery from saturation in cones lacking the 9-methyl group after exposure to bright (>0.1% visual pigment photoactivated) but not dim light. A mathematical model of the turn-off process of phototransduction revealed that the slower recovery of photoresponse can be explained by slower Meta decay of 9-demethyl visual pigment. These results demonstrate that the 9-methyl group of retinal is required for steric chromophore–opsin interactions that favor both the rapid decay of Meta II and the rapid response recovery after exposure to bright light in red-sensitive cones.     

Turning cones off: the role of the 9-methyl group of retinal in red cones

Our ability to see in bright light depends critically on the rapid rate at which cone photoreceptors detect and adapt to changes in illumination. This is achieved, in part, by their rapid response termination. In this study, we investigate the hypothesis that this rapid termination of the response in red cones is dependent on interactions between the 9-methyl group of retinal and red cone opsin, which are required for timely metarhodopsin (Meta) II decay. We used single-cell electrical recordings of flash responses to assess the kinetics of response termination and to calculate guanylyl cyclase (GC) rates in salamander red cones containing native visual pigment as well as visual pigment regenerated with 11-cis 9-demethyl retinal, an analogue of retinal in which the 9-methyl group is missing. After exposure to bright light that photoactivated more than approximately 0.2% of the pigment, red cones containing the analogue pigment had a slower recovery of both flash response amplitudes and GC rates (up to 10 times slower at high bleaches) than red cones containing 11-cis retinal. This finding is consistent with previously published biochemical data demonstrating that red cone opsin regenerated in vitro with 11-cis 9-demethyl retinal exhibited prolonged activation as a result of slowed Meta II decay. Our results suggest that two different mechanisms regulate the recovery of responsiveness in red cones after exposure to light. We propose a model in which the response recovery in red cones can be regulated (particularly at high light intensities) by the Meta II decay rate if that rate has been inhibited. In red cones, the interaction of the 9-methyl group of retinal with opsin promotes efficient Meta II decay and, thus, the rapid rate of recovery.     

Formation of Meta III during the decay of activated rhodopsin proceeds via Meta I and not via Meta II

Thermal isomerization of the retinal Schiff base C=N double bond is known to trigger the decay of rhodopsin's Meta I/Meta II photoproduct equilibrium to the inactive Meta III state [Vogel, R., Siebert, F., Mathias, G., Tavan, P., Fan, G., and Sheves, M. (2003) Biochemistry 42, 9863-9874]. Previous studies have indicated that the transition to Meta III does not occur under conditions that strongly favor the active state Meta II but requires a residual amount of Meta I in the initial photoproduct equilibrium. In this study we show that the triggering event, the thermal isomerization of the protonated Schiff base, is independent of the presence of Meta II and occurs even under conditions where the transition to Meta II is completely prevented. We have examined two examples in which the transitions from Lumi to Meta I or from Meta I to Meta II are blocked. This was achieved using dry films of rhodopsin and rhodopsin reconstituted into rather rigid lipid bilayers. In both cases, the resulting fully inactive room temperature photoproducts decay specifically by thermal isomerization of the protonated Schiff base C=N double bond to an all-trans 15-syn chromophore isomer, corresponding to that of Meta III. This thermal isomerization becomes less efficient as the conformation of the respective photoproduct approaches that of Meta II and is fully absent in a pure Meta II state. These results indicate that the decay of the Meta I/Meta II photoproduct equilibrium to Meta III proceeds via Meta I and not via Meta II.     

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 pK _a 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 pK _a 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.     

Salt dependence of the formation and stability of the signaling state in G protein-coupled receptors: evidence for the involvement of the Hofmeister effect

We studied the salt dependence of both the stability and the equilibrium of the late photoproducts metarhodopsin I (MI) and II (MII) of the artificial visual pigment 9-demethyl rhodopsin (9dm-Rho). In the photoproducts of 9dm-Rho, all-trans-9-demethyl retinal acts only as a partial agonist, enabling us to study the photoproduct equilibrium of the pigment both in membranes and in detergent micelles. Chloride, bromide, and phosphate salts shift this equilibrium from the inactive MI to the active MII receptor conformation both in native membranes and even more with purified pigment in detergent micelles. In the presence of these salts, the induced MII state seems to be structurally intact, as judged by Fourier transform infrared (FTIR) and UV-vis spectroscopy. In the long term, however, we observe an increased instability of the photoproducts and a change in the decay pathways. Both MII enhancement and destabilization are particularly pronounced with the strong chaotropic salts KI and KSCN. The results fit into the framework of the Hofmeister effect and are assigned to an increased solvation of the peptide moiety of the solvent-exposed domains, their resulting partial disordering favoring MII over MI. In this picture, increased solvation also affects helix-helix interactions, thereby leading to a structural instability of the protein in the long term. The reported influences of salts on conformation and stability of this membrane protein are likely to be general and may therefore also apply to other transmembrane proteins and particularly to other G protein-coupled receptors.     

Signaling states of rhodopsin. Retinal provides a scaffold for activating proton transfer switches

The G-protein-coupled receptor rhodopsin is activated by photoconversion of its covalently bound ligand 11-cis-retinal to the agonist all-trans-retinal. After light-induced isomerization and early photointermediates, the receptor reaches a G-protein-dependent equilibrium between active and inactive conformations distinguished by the protonation of key opsin residues. In this report, we study the role of the 9-methyl group of retinal, one of the crucial steric determinants of light activation. We find that when this group is removed, the protonation equilibrium is strongly shifted to the inactive conformation. The residually formed active species is very similar to the active form of normal rhodopsin, metarhodopsin II. It has a deprotonated Schiff base, binds to the retinal G-protein transducin, and is favored at acidic pH. Our data show that the normal proton transfer reactions are inhibited in 9-demethyl rhodopsin but are still mandatory for receptor activation. We propose that retinal and its 9-methyl group act as a scaffold for opsin to adjust key proton donor and acceptor side chains for the proton transfer reactions that stabilize the active conformation. The mechanism may also be applicable to related receptors and may thus explain the partial agonism of certain ligands.     

Constraints of the 9-methyl group binding pocket of the rhodopsin chromophore probed by 9-halogeno substitution

Sterical constraints of the 9-methyl-binding pocket of the rhodopsin chromophore are probed using retinal analogues carrying substituents of increasing size at the 9 position (H, F, Cl, Br, CH(3), and I). The corresponding 11-Z retinals were employed to investigate formation of photosensitive pigment, and the primary photoproduct was identified by Fourier transform infrared difference spectroscopy. In addition, any effects of cumulative strain were studied by introduction of the 9-Z configuration and/or the alpha-retinal ring structure.Our results show that the 9-F analogue still can escape from the 9-methyl-binding pocket and that its photochemistry behaves very similar to the 9-demethyl analogue. The 9-Cl and 9-Br analogues behave very similar to the native 9-methyl pigments, but the 9-I retinal does not fit very well and shows poor pigment formation. This puts an upper limit on the radial dimension of the 9-methyl pocket at 0.45-0.50 nm. Introduction of the alpha-retinal ring constraint in the 11-Z series results in cumulative strain, because the 9-I and 9-Br derivatives cannot bind to generate a photopigment. The 9-Z configuration can partially compensate for the additional alpha-retinal strain. The corresponding 9-Br analogue does form a photopigment, and the other derivatives give increased photopigment yields compared to the corresponding 11-Z derivatives. In fact, 9-Z-alpha-retinal would be an interesting candidate for retinal supplementation studies. Our data provide direct support for the concept that the 9-methyl group is an important determinant in ligand anchoring and activation of the protein and in general agree with a three-point interaction model involving the ring, 9-methyl group, and aldehyde function.     

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 changes in lumirhodopsin and metarhodopsin I studied by their photoreactions at 77 K

The functional process of rhodopsin is initiated by cis-trans photoisomerization of the retinal chromophore. One of the primary intermediates, bathorhodopsin (Batho), is stable at 77 K, and structural changes in Batho are limited around the chromophore. Then, relaxation of Batho leads to helix opening at the cytoplasmic surface in metarhodopsin II (Meta II), which allows activation of a G protein transducin. Two intermediates, lumirhodopsin (Lumi) and metarhodopsin I (Meta I), appear between Batho and Meta II, and can be stabilized at 200 and 240 K, respectively. A photoaffinity labeling experiment reported that formation of Lumi accompanied flip-over of the beta-ionone ring of the retinal chromophore so that the ring portion was attached to Ala169 of helix IV [Borhan, B., Souto, M. L., Imai, H., Shichida, Y., and Nakanishi, K. (2000) Science 288, 2209-2212]. According to the crystal structure of bovine rhodopsin, the distance between the labeled C3 atom of the chromophore and Ala169 was >15 A [Palczewski, K., Kumasaka, T., Hori, T., Behnke, C. A., Motoshima, H., Fox, B. A., Le Trong, I., Teller, D. C., Okada, T., Stenkamp, R. E., Yamamoto, M., and Miyano, M. (2000) Science 289, 739-745]. These facts suggest that global protein structural changes such as helix motions take place in Lumi. In the study presented here, Lumi and Meta I are illuminated at 77 K, and protein structural changes are probed by Fourier transform infrared (FTIR) spectroscopy. We found that Lumi can be photoconverted to rhodopsin at 77 K from the IR spectral analysis of the photoproducts of Lumi. In contrast, more complex spectra were obtained for the photoproducts of Meta I at 77 K, implying that the protein structure of Meta I is considerably altered so as not to be reverted to the original state at 77 K. Thus, these photoreaction experiments with Lumi and Meta I at 77 K suggested the presence of global protein structural changes in the process between them. We concluded that the helix motions do not occur at Lumi, but at Meta I, and the flip-over of the beta-ionone ring reported by the photoaffinity labeling takes place through the specific reaction channel without a change in the global structure.     

Photoreactions of metarhodopsin III

Meta III is an inactive intermediate thermally formed following light activation of the visual pigment rhodopsin. It is produced from the Meta I/Meta II photoproduct equilibrium of rhodopsin by a thermal isomerization of the protonated Schiff base C=N bond of Meta I, and its chromophore configuration is therefore all-trans 15-syn. In contrast to the dark state of rhodopsin, which catalyzes exclusively the cis to trans isomerization of the C11=C12 bond of its 11-cis 15-anti chromophore, Meta III does not acquire this photoreaction specificity. Instead, it allows for light-dependent syn to anti isomerization of the C15=N bond of the protonated Schiff base, yielding Meta II, and for trans to cis isomerizations of C11=C12 and C9=C10 of the retinal polyene, as shown by FTIR spectroscopy. The 11-cis and 9-cis 15-syn isomers produced by the latter two reactions are not stable, decaying on the time scale of few seconds to dark state rhodopsin and isorhodopsin by thermal C15=N isomerization, as indicated by time-resolved FTIR methods. Flash photolysis of Meta III produces therefore Meta II, dark state rhodopsin, and isorhodopsin. Under continuous illumination, the latter two (or its unstable precursors) are converted as well to Meta II by presumably two different mechanisms.     

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)     

Electrogenic transport properties of bacteriorhodopsin containing chemically modified retinal analogues

The electrical activity of bacteriorhodopsin (BR) containing the 13-substituted retinal analogues 13-demethyl and 13-methoxy as well as the naturally occurring retinal carrying a methyl group at C13 is compared. White membrane patches reconstituted with the different retinals are attached to a black lipid membrane, and the dependency of the photocurrent on light intensity is measured. This allows a comparison of the overall photocycle time and the number of protons transported per cycle for the various preparations. From previous work (Gärtner, W., Towner, P., Hopf, H. and Oesterhelt, D. (1983) Biochem. 22, 2637–2644, see also Gärtner, W. and Oesterhelt, D., unpublished data) the equilibrium isomeric distribution (all-trans and 13-cis) of the different retinals in the binding site is known. Taking into account that only all-trans retinal BR contributes to the pumping activity (Fahr, A. and Bamberg, E. (1982) FEBS Lett. 140, 251–253), it is shown, that the cycle time for the modified BRs is moderately changed, whereas the number of protons transported per cycle and transporting all-trans BR molecule is not affected by the substituent. It is concluded, that substituting the methyl group at position 13 of the retinal molecule by a hydrogen atom or a methoxy group only slightly affects the pumping activity of the trans-photocycle, but rather controls the biological function of BR via the equilibrium isomeric distribution of the retinal molecule in the binding site.     

Deactivation and proton transfer in light-induced metarhodopsin II/metarhodopsin III conversion: a time-resolved fourier transform infrared spectroscopic study

Vertebrate rhodopsin shares with other retinal proteins the 11-cis-retinal chromophore and the light-induced 11-cis/trans isomerization triggering its activation pathway. However, only in rhodopsin the retinylidene Schiff base bond to the apoprotein is eventually hydrolyzed, making a complex regeneration pathway necessary. Metabolic regeneration cannot be short-cut, and light absorption in the active metarhodopsin (Meta) II intermediate causes anti/syn isomerization around the retinylidene linkage rather than reversed trans/cis isomerization. A new deactivating pathway is thereby triggered, which ends in the Meta III "retinal storage" product. Using time-resolved Fourier transform infrared spectroscopy, we show that the identified steps of receptor activation, including Schiff base deprotonation, protein structural changes, and proton uptake by the apoprotein, are all reversed. However, Schiff base reprotonation is much faster than the activating deprotonation, whereas the protein structural changes are slower. The final proton release occurs with pK approximately 4.5, similar to the pK of a free Glu residue and to the pK at which the isolated opsin apoprotein becomes active. A forced deprotonation, equivalent to the forced protonation in the activating pathway, which occurs against the unfavorable pH of the medium, is not observed. This explains properties of the final Meta III product, which displays much higher residual activity and is less stable than rhodopsin arising from regeneration with 11-cis-retinal. We propose that the anti/syn conversion can only induce a fast reorientation and distance change of the Schiff base but fails to build up the full set of dark ground state constraints, presumably involving the Glu(134)/Arg(135) cluster.     

Asp83, Glu113 and Glu134 are not specifically involved in Schiff base protonation or wavelength regulation in bovine rhodopsin

Site-specific mutagenesis was employed to investigate the proposed contribution of proton-donating residues (Glu, Asp) in the membrane domains of bovine rhodopsin to protonation of the Schiff base-linking protein and chromophore or to wavelength modulation of this visual pigment. Three point-mutations were introduced to replace the highly conserved residues Asp83 by Asn (D83N), Glu113 by Gln (E113 Q) or Glu134 by Asp (E134D), respectively. All 3 substitutions had only marginal effects on the spectral properties of the final pigment (less than or equal to 3 nm blue-shift relative to native rhodopsin). Hence, none of these residues by itself is specifically involved in Schiff base protonation or wavelength modulation of bovine rhodopsin.     

Elucidating the exact role of engineered CRABPII residues for the formation of a retinal protonated Schiff base

Cellular Retinoic Acid Binding Protein II (CRABPII) has been reengineered to specifically bind and react with all‐trans‐retinal to form a protonated Schiff base. Each step of this process has been dissected and four residues (Lys132, Tyr134, Arg111, and Glu121) within the CRABPII binding site have been identified as crucial for imine formation and/or protonation. The precise role of each residue has been examined through site directed mutagenesis and crystallographic studies. The crystal structure of the R132K:L121E‐CRABPII (PDB‐3I17) double mutant suggests a direct interaction between engineered Glu121 and the native Arg111, which is critical for both Schiff base formation and protonation. Proteins 2009. © 2009 Wiley‐Liss, Inc.     

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.     

Origin and consequences of steric strain in the rhodopsin binding pocket

To study the origin and the effects of steric strain on the chromophore conformation in rhodopsin, we have performed quantum-mechanical calculations on the wild-type retinal chromophore and four retinal derivatives, 13-demethyl-, 10-methyl-13-demethyl-, 10-methyl-, and 9-demethylretinal. For the dynamics of the whole protein, a combined quantum mechanics/molecular mechanics method (DFTB/CHARMM) was used and for the calculation of excited-state properties the nonempirical CASSCF/CASPT2 method. After relaxation inside the protein, all chromophores show significant nonplanar distortions from C10 to C13, most strongly for 10-methylretinal and least pronounced for 9-demethylretinal. In all five cases, the dihedral angle of the C10-C11=C12-C13 bond is negative which attests to the strong chiral discrimination exerted by the protein pocket. The calculations show that the nonplanar distortion of the chromophore, including the sense of rotation, is caused by a combination of two effects: the fitting of both ends to the protein matrix which imposes a distance constraint and the bonding arrangement at the Schiff base terminus. With both the counterion Glu113 and Lys296 displaced off the plane of the chromophore, their binding to N16 exerts a torque on the chromophore. As a result, the polyene chain, from N16 to C13, is twisted in a clockwise manner against the remaining part of the chromophore, leading to a C11=C12 bond with the observed negative dihedral angle. Shifts of the absorption maxima are reproduced correctly, in particular, the red shift of the 10-methyl and the strong blue shift of the 9-demethyl analogue relative to the wild type. Calculated positive rotatory strengths of the alpha-CD bands are in agreement with the calculated absolute conformation of the mutant chromophores.