1H and 13C MAS NMR evidence for pronounced ligand-protein interactions involving the ionone ring of the retinylidene chromophore in rhodopsin (original) (raw)
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Biochemistry Usa, 1999
Rhodopsin is the G-protein coupled photoreceptor that initiates the rod phototransduction cascade in the vertebrate retina. Using specific isotope enrichment and magic angle spinning (MAS) NMR, we examine the spatial structure of the C10-C11dC12-C13-C20 motif in the native retinylidene chromophore, its 10-methyl analogue, and the predischarge photoproduct metarhodopsin-I. For the rhodopsin study 11-Z-[10,20-13 C 2 ]-and 11-Z-[11,20-13 C 2 ]-retinal were synthesized and incorporated into bovine opsin while maintaining a natural lipid environment. The ligand is covalently bound to Lys 296 in the photoreceptor. The C10-C20 and C11-C20 distances were measured using a novel 1-D CP/MAS NMR rotational resonance experimental procedure that was specifically developed for the purpose of these measurements [Verdegem, P. J. E., Helmle, M., Lugtenburg, J., and de Groot, H. J. M. (1997) J. Am. Chem. Soc. 119, 169]. We obtain r 10,20 ) 0.304 ( 0.015 nm and r 11,20 ) 0.293 ( 0.015 nm, which confirms that the retinylidene is 11-Z and shows that the C10-C13 unit is conformationally twisted. The corresponding torsional angle is about 44°as indicated by Car-Parrinello modeling studies. To increase the nonplanarity in the chromophore, 11-Z-[10,20-13 C 2 ]-10-methylretinal and 11-Z-[(10-CH 3 ),13-13 C 2 ]-10-methylretinal were prepared and incorporated in opsin. For the resulting analogue pigment r 10,20 ) 0.347 ( 0.015 nm and r (10-CH 3 ),13 ) 0.314 ( 0.015 nm were obtained, consistent with a more distorted chromophore. The analogue data are in agreement with the induced fit principle for the interaction of opsin with modified retinal chromophores. Finally, we determined the intraligand distances r 10,20 and r 11,20 also for the photoproduct metarhodopsin-I, which has a relaxed all-E structure. The results (r 10,20 g 0.435 nm and r 11,20 ) 0.283 ( 0.015 nm) fully agree with such a relaxed all-E structure, which further validates the 1-D rotational resonance technique for measuring intraligand distances and probing ligand structure. As far as we are aware, these results represent the first highly precise distance determinations in a ligand at the active site of a membrane protein. Overall, the MAS NMR data indicate a tight binding pocket, well defined to bind specifically only one enantiomer out of four possibilities and providing a steric complement to the chromophore in an ultrafast (∼200 fs) isomerization process. †
Biochemistry, 2004
Rhodopsin is the photosensitive protein of the rod photoreceptor in the vertebrate retina and is a paradigm for the superfamily of G-protein-coupled receptors (GPCRs). Natural rhodopsin contains an 11-cis-retinylidene chromophore. We have prepared the 9-cis analogue isorhodopsin in a natural membrane environment using uniformly 13 C-enriched 9-cis retinal. Subsequently, we have determined the complete 1 H and 13 C assignments with ultra-high field solid-state magic angle spinning NMR. The 9-cis substrate conforms to the opsin binding pocket in isorhodopsin in a manner very similar to that of the 11-cis form in rhodopsin, but the NMR data reveal an improper fit of the 9-cis chromophore in this binding site. We introduce the term "induced misfit" to describe this event. Downfield proton NMR ligation shifts (∆σ lig H > 1 ppm) are observed for the 16,17,19-H and nearby protons of the ionone ring and for the 9-methyl protons. They provide converging evidence for global, nonspecific steric interactions between the chromophore and protein, and contrast with the specific interactions over the entire ionone ring and its substituents detected for rhodopsin. The ∆σ lig C pattern of the polyene chain confirms the positive charge delocalization in the polyene associated with the protonation of the Schiff base nitrogen. In line with the misalignment of the ionone ring, an additional and anomalous perturbation of the 13 C response is detected in the region of the 9-cis bond. This provides evidence for strain in the isomerization region of the polyene and supports the hypothesis that perturbation of the conjugation around the cis bond induced by the protein environment assists the selective photoisomerization. H , isotropic proton shift of the chromophore; σlig C , isotropic carbon shift of the chromophore; σpSB H , isotropic proton shift of the pSB model compound; σpSB C , isotropic carbon shift of the pSB model compound; σlip H , isotropic proton shift of the phospholipids; σlip C , isotropic carbon shift of the phospholipids; ∆σlig H , proton NMR ligation shift; ∆σlig C , carbon NMR ligation shift; ∆σlig H , normalized proton NMR ligation shift; ∆σ lig C , normalized carbon NMR ligation shift; ∆σ total , sum of the ∆σlig C values of the 13 C of the polyene chain.
Journal of Molecular Biology, 2007
Rhodopsin is a prototype for G protein-coupled receptors (GPCRs) that are implicated in many biological responses in humans. A site-directed 2 H NMR approach was used for structural analysis of retinal within its binding cavity in the dark and pre-activated meta I states. Retinal was labeled with 2 H at the C5, C9, or C13 methyl groups by total synthesis, and was used to regenerate the opsin apoprotein. Solid-state 2 H NMR spectra were acquired for aligned membranes in the low-temperature lipid gel phase versus the tilt angle to the magnetic field. Data reduction assumed a static uniaxial distribution, and gave the retinylidene methyl bond orientations plus the alignment disorder (mosaic spread). The darkstate 2 H NMR structure of 11-cis-retinal shows torsional twisting of the polyene chain and the β-ionone ring. The ligand undergoes restricted motion, as evinced by order parameters of ≈ 0.9 for the spinning C-C 2 H 3 groups, with off-axial fluctuations of ≈ 15°. Retinal is accommodated within the rhodopsin binding pocket with a negative pre-twist about the C11 = C12 double bond that explains its rapid photochemistry and the trajectory of 11-cis to trans isomerization. In the cryo-trapped meta I state, the 2 H NMR structure shows a reduction of the polyene strain, while torsional twisting of the β-ionone ring is maintained. Distortion of the retinal conformation is interpreted through substituent control of receptor activation. Steric hindrance between trans retinal and Trp265 can trigger formation of the subsequent activated meta II state. Our results are pertinent to quantum and molecular mechanics simulations of ligands bound to GPCRs, and illustrate how 2 H NMR can be applied to study their biological mechanisms of action.
Biochemistry, 2001
C 10 ]Retinal prepared by total synthesis is reconstituted with opsin to form rhodopsin in the natural lipid membrane environment. The 13 C shifts are assigned with magic angle spinning NMR dipolar correlation spectroscopy in a single experiment and compared with data of singly labeled retinylidene ligands in detergent-solubilized rhodopsin. The use of multispin labeling in combination with 2-D correlation spectroscopy improves the relative accuracy of the shift measurements. We have used the chemical shift data to analyze the electronic structure of the retinylidene ligand at three levels of understanding: (i) by specifying interactions between the 13 C-labeled ligand and the G-protein-coupled receptor target, (ii) by making a charge assessment of the protonation of the Schiff base in rhodopsin, and (iii) by evaluating the total charge on the carbons of the retinylidene chromophore. In this way it is shown that a conjugation defect is the predominant ground-state property governing the molecular electronics of the retinylidene chromophore in rhodopsin. The cumulative chemical shifts at the odd-numbered carbons (∆σ odd ) of 11-Z-protonated Schiff base models relative to the unprotonated Schiff base can be used to measure the extent of delocalization of positive charge into the polyene. For a series of 11-Z-protonated Schiff base models and rhodopsin, ∆σ odd appears to correlate linearly with the frequency of maximum visible absorption. Since rhodopsin has the largest value of ∆σ odd , the data contribute to existing and converging spectroscopic evidence for a complex counterion stabilizing the protonated Schiff base in the binding pocket.
The Ring of the Rhodopsin Chromophore in a Hydrophobic Activation Switch Within the Binding Pocket
Journal of Molecular Biology, 2004
The current view that the beta-ionone ring of the rhodopsin chromophore vacates its binding pocket within the protein early in the photocascade has been adopted in efforts to provide structural models of photoreceptor activation. This event casts doubt on the ability of this covalently bonded ligand to participate directly in later stages involving activation of the photoreceptor and it is difficult to translate into predictions for the activation of related G protein-coupled receptors by diffusable ligands (e.g. neurotransmitters). The binding pocket fixes the formally equivalent pair of ring methyl groups (C16/C17) in different orientations that can be distinguished easily by (13)C NMR. Solid-state NMR observations on C16 and C17 are reported here that show instead that the ring is retained with strong selective interactions within the binding site into the activated state. We further show how increased steric interactions for this segment in the activated receptor can be explained by adjustment in the protein structure around the ring whilst it remains in its original location. This describes a plausible role for the ring in operating a hydrophobic switch from within the aromatic cluster of helix 6 of rhodopsin, which is coupled to electronic changes within the receptor through water-mediated, hydrogen-bonded networks between the conserved residues in G protein-coupled receptors.
Journal of The American Chemical Society, 2004
We have obtained carbon-carbon bond length data for the functional retinylidene chromophore of rhodopsin, with a spatial resolution of 3 pm. The very high resolution was obtained by performing doublequantum solid-state NMR on a set of noncrystalline isotopically labelled bovine rhodopsin samples. We detected localized perturbations of the carbon-carbon bond lengths of the retinylidene chromophore. The observations are consistent with a model in which the positive charge of the protonated Schiff base penetrates into the polyene chain and partially concentrates around the C13 position. This coincides with the proximity of a water molecule located between the glutamate-181 and serine-186 residues of the second extracellular loop, which is folded back into the transmembrane region. These measurements support the hypothesis that the polar residues of the second extracellular loop and the associated water molecule assist the rapid selective photoisomerization of the retinylidene chromophore by stabilizing a partial positive charge in the center of the polyene chain.
Biochemistry, 2001
In the absence of a high-resolution diffraction structure, the orientation and conformation of the protonated Schiffs base retinylidinium chromophore of rhodopsin within the opsin matrix has been the subject of much speculation. There have been two recent reliable and precise NMR results that bear on this issue. One involves a determination of the C20-C10 and C20-C11 distances by Verdegem et al. [Biochemistry 38, 11316-11324 (1999)]. The other is the determination of the orientation of the methine C to methyl group vectors C5-C18, C9-C19, and C13-C20 relative to the membrane normal by Gröbner et al. [Nature 405 (6788), 810-813 ]. Using molecular orbital methods that include extensive configuration interaction, we have determined what we propose to be the minimum energy conformation of this chromophore. The above NMR results permit us to check this structure in the C10-C11dC12-C13 region and then to check the global structure via the relative orientation of the three C18, C19, and C20 methyl groups. This method provides a detailed structure and also the orientation for the retinyl chromophore relative to the membrane normal and argues strongly that the protein does not appreciably alter the chromophore geometry from its minimum energy configuration that is nearly planar s-trans at the 6-7 bond. Finally, the chromophore structure and orientation presented in the recently published X-ray diffraction structure is compared with our proposed structure and with the deuterium NMR results. .
Dynamic Structure of Retinylidene Ligand of Rhodopsin Probed by Molecular Simulations
Journal of Molecular Biology, 2007
Rhodopsin is currently the only available atomic-resolution template for understanding biological functions of the G protein-coupled receptor (GPCR) family. The structural basis for the phenomenal dark state stability of 11-cis-retinal bound to rhodopsin and its ultrafast photoreaction are active topics of research. In particular, the β-ionone ring of the retinylidene inverse agonist is crucial for the activation mechanism. We analyzed a total of 23 independent, 100 ns all-atom molecular dynamics simulations of rhodopsin embedded in a lipid bilayer in the microcanonical (N,V,E) ensemble. Analysis of intramolecular fluctuations predicts hydrogen-out-of-plane (HOOP) wagging modes of retinal consistent with those found in Raman vibrational spectroscopy. We show that sampling and ergodicity of the ensemble of simulations are crucial for determining the distribution of conformers of retinal bound to rhodopsin. The polyene chain is rigidly locked into a single, twisted conformation, consistent with the function of retinal as an inverse agonist in the dark state. Most surprisingly, the β-ionone ring is mobile within its binding pocket; interactions are non-specific and the cavity is sufficiently large to enable structural heterogeneity. We find that retinal occupies two distinct conformations in the dark state, contrary to most previous assumptions. The β-ionone ring can rotate relative to the polyene chain, thereby populating both positively and negatively twisted 6-s-cis enantiomers. This result, while unexpected, strongly agrees with experimental solid-state 2 H NMR spectra. Correlation analysis identifies the residues most critical to controlling mobility of retinal; we find that Trp265 moves away from the ionone ring prior to any conformational transition. Our findings reinforce how molecular dynamics simulations can challenge conventional assumptions for interpreting experimental data, especially where existing models neglect conformational fluctuations.
Photochemistry and Photobiology, 2009
Solid-state NMR spectroscopy gives a powerful avenue for investigating G protein-coupled receptors and other integral membrane proteins in a native-like environment. This article reviews the use of solid-state 2 H NMR to study the retinal cofactor of rhodopsin in the dark state as well as the meta I and meta II photointermediates. Site-specific 2 H NMR labels have been introduced into three regions (methyl groups) of retinal that are crucially important for the photochemical function of rhodopsin. Despite its phenomenal stability 2 H NMR spectroscopy indicates retinal undergoes rapid fluctuations within the protein binding cavity. The spectral lineshapes reveal the methyl groups spin rapidly about their three-fold (C 3 ) axes with an order parameter for the off-axial motion of S C3 % 0:9: For the dark state, the 2 H NMR structure of 11-cis-retinal manifests torsional twisting of both the polyene chain and the b-ionone ring due to steric interactions of the ligand and the protein. Retinal is accommodated within the rhodopsin binding pocket with a negative pretwist about the C11=C12 double bond. Conformational distortion explains its rapid photochemistry and reveals the trajectory of the 11-cis to trans isomerization. In addition, 2 H NMR has been applied to study the retinylidene dynamics in the dark and light-activated states. Upon isomerization there are drastic changes in the mobility of all three methyl groups. The relaxation data support an activation mechanism whereby the b-ionone ring of retinal stays in nearly the same environment, without a large displacement of the ligand. Interactions of the b-ionone ring and the retinylidene Schiff base with the protein transmit the force of the retinal isomerization. Solid-state 2 H NMR thus provides information about the flow of energy that triggers changes in hydrogen-bonding networks and helix movements in the activation mechanism of the photoreceptor. †This paper is part of the