Changes in interhelical hydrogen bonding upon rhodopsin activation

Hydrogen bonding interactions between transmembrane helices stabilize the visual pigment rhodopsin in an inactive conformation in the dark. The crystal structure of rhodopsin has previously revealed that Glu122 and Trp126 on transmembrane helix H3 form a complex hydrogen bonding network with Tyr206 and His211 on H5, while the indole nitrogen of Trp265 on H6 forms a water-mediated hydrogen bond with Asn302 on H7. Here, we use solid-state magic angle spinning NMR spectroscopy to probe the changes in hydrogen bonding upon rhodopsin activation. The NMR chemical shifts of 15N-labeled tryptophan are consistent with the indole nitrogens of Trp126 and Trp265 becoming more weakly hydrogen bonded between rhodopsin and metarhodopsin II. The NMR chemical shifts of 15N-labeled histidine show that His211 is neutral; the unprotonated imidazole nitrogen is not coordinated to zinc in rhodopsin and becomes more strongly hydrogen bonded in metarhodopsin II. Moreover, measurements of rhodopsin containing 13C-labeled histidine show that a strong hydrogen bond between the side-chain of Glu122 and the backbone carbonyl of His211 is disrupted in metarhodopsin II. The implications of these observations for the activation mechanism of rhodopsin are discussed.     

Light Activation of Rhodopsin: Insights from Molecular Dynamics Simulations Guided by Solid-State NMR Distance Restraints

Structural restraints provided by solid-state NMR measurements of the metarhodopsin II intermediate are combined with molecular dynamics simulations to help visualize structural changes in the light activation of rhodopsin. Since the timescale for the formation of the metarhodopsin II intermediate (> 1 ms) is beyond that readily accessible by molecular dynamics, we use NMR distance restraints derived from ¹³C dipolar recoupling measurements to guide the simulations. The simulations yield a working model for how photoisomerization of the 11-cis retinylidene chromophore bound within the interior of rhodopsin is coupled to transmembrane helix motion and receptor activation. The mechanism of activation that emerges is that multiple switches on the extracellular (or intradiscal) side of rhodopsin trigger structural changes that converge to disrupt the ionic lock between helices H3 and H6 on the intracellular side of the receptor.     

Retinal dynamics during light activation of rhodopsin revealed by solid-state NMR spectroscopy

Rhodopsin is a canonical member of class A of the G protein-coupled receptors (GPCRs) that are implicated in many of the drug interventions in humans and are of great pharmaceutical interest. The molecular mechanism of rhodopsin activation remains unknown as atomistic structural information for the active metarhodopsin II state is currently lacking. Solid-state ²H NMR constitutes a powerful approach to study atomic-level dynamics of membrane proteins. In the present application, we describe how information is obtained about interactions of the retinal cofactor with rhodopsin that change with light activation of the photoreceptor. The retinal methyl groups play an important role in rhodopsin function by directing conformational changes upon transition into the active state. Site-specific ²H labels have been introduced into the methyl groups of retinal and solid-state ²H NMR methods applied to obtain order parameters and correlation times that quantify the mobility of the cofactor in the inactive dark state, as well as the cryotrapped metarhodopsin I and metarhodopsin II states. Analysis of the angular-dependent ²H NMR line shapes for selectively deuterated methyl groups of rhodopsin in aligned membranes enables determination of the average ligand conformation within the binding pocket. The relaxation data suggest that the β-ionone ring is not expelled from its hydrophobic pocket in the transition from the pre-activated metarhodopsin I to the active metarhodopsin II state. Rather, the major structural changes of the retinal cofactor occur already at the metarhodopsin I state in the activation process. The metarhodopsin I to metarhodopsin II transition involves mainly conformational changes of the protein within the membrane lipid bilayer rather than the ligand. The dynamics of the retinylidene methyl groups upon isomerization are explained by an activation mechanism involving cooperative rearrangements of extracellular loop E2 together with transmembrane helices H5 and H6. These activating movements are triggered by steric clashes of the isomerized all-trans retinal with the β4 strand of the E2 loop and the side chains of Glu¹²² and Trp²⁶⁵ within the binding pocket. The solid-state ²H NMR data are discussed with regard to the pathway of the energy flow in the receptor activation mechanism.     

Engineering a "steric doorstop" in rhodopsin: converting an inverse agonist to an agonist

The crystal structures of rhodopsin depict the inactive conformation of rhodopsin in the dark. The 11-cis retinoid chromophore, the inverse agonist holding rhodopsin inactive, is well-resolved. Thr118 in helix 3 is the closest amino acid residue next to the 9-methyl group of the chromophore. The 9-methyl group of retinal facilitates the transition from an inactive metarhodopsin I to the active metarhodopsin II intermediate. In this study, a site-specific mutation of Thr118 to the bulkier Trp was made with the idea to induce an active conformation of the protein. The data indicate that such a mutation does indeed result in an active protein that depends on the presence of the ligand, specifically the 9-methyl group. As a result of this mutation, 11-cis retinal has been converted to an agonist. The apoprotein form of this mutant is no more active than the wild-type apoprotein. However, unlike wild-type rhodopsin, the covalent linkage of the ligand can be attacked by hydroxylamine in the dark. The combination of the Thr118Trp mutation and the 9-methyl group of the chromophore behaves as a "steric doorstop" holding the protein in an open and active conformation.     

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.     

Structural and functional role of helices I and II in rhodopsin. A novel interplay evidenced by mutations at Gly-51 and Gly-89 in the transmembrane domain

The naturally occurring mutations G51A and G51V in transmembrane helix I and G89D in the transmembrane helix II of rhodopsin are associated with the retinal degenerative disease autosomal dominant retinitis pigmentosa. To probe the orientation and packing of helices I and II a number of replacements at positions 51 and 89 were prepared by using site-directed mutagenesis, and the corresponding proteins expressed in COS-1 cells were characterized. Mutations at position 51 (G51V and G51L) bound retinal like wild-type rhodopsin but had thermally destabilized structures in the dark, altered photobleaching behavior, destabilized metarhodopsin II active conformations, and were severely defective in signal transduction. The effects observed can be correlated with the size of the mutated side chains that would interfere with specific interhelical interaction with Val-300 in helix VII. Mutations at position 89 had sensitivity to charge, as in G89K and G89D mutants, which showed reduced transducin activation. G89K showed a second absorbing species in the UV region at 350 nm, suggesting a charge effect of the introduced lysine. Increased formation of non-active forms of rhodopsin, like metarhodopsin III, may have some influence in the molecular defect underlying retinitis pigmentosa in the mutants studied. At the structural level, the effect of the mutations analyzed can be rationalized assuming a very specific set of tertiary interactions in the interhelical packing of the transmembrane segments of rhodopsin.     

Dipolar assisted rotational resonance NMR of tryptophan and tyrosine in rhodopsin

Two dimensional (2D) solid-state (13)C.(13)C dipolar recoupling experiments are performed on a series of model compounds and on the visual pigment rhodopsin to establish the most effective method for long range distance measurements in reconstituted membrane proteins. The effects of uniform labeling, inhomogeneous B(1) fields, relaxation and dipolar truncation on cross peak intensity are investigated through NMR measurements of simple amino acid and peptide model compounds. We first show that dipolar assisted rotational resonance (DARR) is more effective than RFDR in recoupling long-range dipolar interactions in these model systems. We then use DARR to establish (13)C-(13)C correlations in rhodopsin. In rhodopsin containing 4'-(13)C-Tyr and 8,19-(13)C retinal, we observe two distinct tyrosine-to-retinal correlations in the DARR spectrum. The most intense cross peak arises from a correlation between Tyr268 and the retinal 19-(13)CH(3), which are 4.8 A apart in the rhodopsin crystal structure. A second cross peak arises from a correlation between Tyr191 and the retinal 19-(13)CH(3), which are 5.5 A apart in the crystal structure. These data demonstrate that long range (13)C em leader (13)C correlations can be obtained in non-crystalline integral membrane proteins reconstituted into lipid membranes containing less than 150 nmoles of protein. In rhodopsin containing 2-(13)C Gly121 and U-(13)C Trp265, we do not observe a Trp-Gly cross peak in the DARR spectrum despite their close proximity (3.6 A) in the crystal structure. Based on model compounds, the absence of a (13)C em leader (13)C cross peak is due to loss of intensity in the diagonal Trp resonances rather than to dipolar truncation.     

Activation of phosphodiesterase by rhodopsin and its analogues

Activation of guanosine 3',5'-cyclic monophosphate (cGMP) phosphodiesterase (EC 3.1.4.35.) in frog rod outer segment membrane by rhodopsin and its analogues was investigated. The Schiff-base linkage between opsin and retinal in rhodopsin was not always necessary for the phosphodiesterase activation. The binding of beta-ionone ring of retinal to a hydrophobic region of opsin was not enough to induce the enzyme activation. A striking photo-activation of the enzyme was induced by photo-isomerization of rhodopsin analogues from cis to trans form. It seems probable that an "expanded" conformation of opsin around the retinylidene chromophore induced by the cis to trans isomerization may be the trigger for the activation of phosphodiesterase. On the other hand, the phosphodiesterase in frog rod outer segment was activated by warming of bathorhodopsin to -12 degrees C and then incubating it at the same temperature. Thus, metarhodopsin II or an earlier intermediate than metarhodopsin II should be a direct intermediate for the enzyme activation.     

Lack of interaction of rhodopsin chromophore with membrane lipids. An electron-electron double resonance study using 14N:15N pairs.

Electron-electron double resonance (ELDOR) has been applied to the study of specific interactions of 15N-spin-labeled stearic acid with the retinal chromophore of a rhodopsin analogue containing a 14N spin-labeled retinal. Both the 5 and 16 spin-labeled stearic acids were incorporated into the lipid bilayer of rod outer segment membranes containing the spin-labeled pigment. No interaction between the 15N and 14N spin-labels was observed in rhodopsin or the metarhodopsin II state with either of these labeled stearic acids. Therefore in this system the ring portion of the chromophore must be highly sequestered from the phospholipid bilayer in both the rhodopsin and metarhodopsin II forms.     

Partial agonism in a G Protein-coupled receptor: role of the retinal ring structure in rhodopsin activation

The visual process in rod cells is initiated by absorption of a photon in the rhodopsin retinal chromophore and consequent retinal cis/trans-isomerization. The ring structure of retinal is thought to be needed to transmit the photonic energy into conformational changes culminating in the active metarhodopsin II (Meta II) intermediate. Here, we demonstrate that cis-acyclic retinals, lacking four carbon atoms of the ring, can activate rhodopsin. Detailed analysis of the activation pathway showed that, although the photoproduct pathway is more complex, Meta II formed with almost normal kinetics. However, lack of the ring structure resulted in a low amount of Meta II and a fast decay of activity. We conclude that the main role of the ring structure is to maintain the active state, thus specifying a mechanism of activation by a partial agonist of the G protein-coupled receptor rhodopsin.     

Probing intramolecular orientations in rhodopsin and metarhodopsin II by polarized infrared difference spectroscopy.

The light-induced conformational changes of rhodopsin, which lead to the formation of the G-protein activating metarhodopsin II intermediate, are studied by polarized attenuated total reflectance infrared difference spectroscopy. Orientations of protein groups as well as the retinylidene chromophore were calculated from the linear dichroism of infrared difference bands. These bands correspond to changes in the vibrational modes of individual molecular groups that are structurally active during receptor activation, i.e., during the rhodopsin to metarhodopsin II transition. The orientation of the transition dipole moments of bands previously assigned to the carboxyl (C=O) groups of Asp83 and Glu113 has been determined. The orientation of specific groups in the retinylidene chromophore has been inferred from the dichroism of the bands associated with the polyene C-C, C=C, and hydrogen-out-of-plane vibrations. Interestingly, the use of polarized infrared light reveals several difference bands in the rhodopsin to metarhodopsin II difference spectrum which were previously undetected, e.g., at 1736 and 939 cm(-1). The latter is tentatively assigned to the hydrogen-out-of-plane mode of the HC(11)=C(12)H segment of the chromophore. Our data suggest a significant change in orientation of this group in the late phase of rhodopsin activation. On the basis of available site-directed mutagenesis data, bands at 1406, 1583, and 1736 cm(-1) are tentatively assigned to Glu134. The main features in the amide regions in the dichroic difference spectrum are discussed in terms of a slight reorientation of helical segments upon receptor activation.     

Structural analysis and dynamics of retinal chromophore in dark and meta I states of rhodopsin from 2H NMR of aligned membranes

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 dark-state (2)H NMR structure of 11-cis-retinal shows torsional twisting of the polyene chain and the beta-ionone ring. The ligand undergoes restricted motion, as evinced by order parameters of approximately 0.9 for the spinning C-C(2)H(3) groups, with off-axial fluctuations of approximately 15 degrees . 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 beta-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.     

Analogue pigment studies of chromophore-protein interactions in metarhodopsins

Several analogue pigments have been prepared containing retinals altered at the cyclohexyl ring or proximal to the aldehyde group in order to examine the role of the chromophore in the formation of the metarhodopsin I and II states of visual pigments. Deletion of the 13-methyl group on the isoprenoid chain did not affect metarhodopsin formation. However, analogue pigments containing chromophores with modified rings did not show the typical absorption changes associated with the metarhodopsin transitions of native or regenerated rhodopsins. In particular, 4-hydroxyretinal pigments did not show clear transitions between the metarhodopsin I and metarhodopsin II states. Pigment formed with an acyclic retinal showed no evidence by absorption spectroscopy of metarhodopsin formation. A retinal altered by substitution of a five-membered ring containing a nitroxide required a more acidic pH than the native pigment for formation of the metarhodopsin II state. ESR data suggest that the ring remains buried within the protein through the metarhodopsin II state. However, the Schiff base linkage is susceptible to hydrolysis of hydroxylamine in the metarhodopsin II state. These data indicate that (1), in the transition from rhodopsin to metarhodopsin II, major protein conformational changes are occurring near the lysine-retinal linkage whereas the ring portion of the chromophore remains deeply buried within the protein and (2) pigment absorptions characteristic of the metarhodopsin I and II states may be due to specific protein-chromophore interactions near the region of the chromophore ring.     

Resonance raman spectroscopy of an ultraviolet-sensitive insect rhodopsin

We present the first visual pigment resonance Raman spectra from the UV-sensitive eyes of an insect, Ascalaphus macaronius (owlfly). This pigment contains 11-cis-retinal as the chromophore. Raman data have been obtained for the acid metarhodopsin at 10 degrees C in both H2O and D2O. The C = N stretching mode at 1660 cm-1 in H2O shifts to 1631 cm-1 upon deuteriation of the sample, clearly showing a protonated Schiff base linkage between the chromophore and the protein. The structure-sensitive fingerprint region shows similarities to the all-trans-protonated Schiff base of model retinal chromophores, as well as to the octopus acid metarhodopsin and bovine metarhodopsin I. Although spectra measured at -100 degrees C with 406.7-nm excitation, to enhance scattering from rhodopsin (lambda max 345 nm), contain a significant contribution from a small amount of contaminants [cytochrome(s) and/or accessory pigment] in the sample, the C = N stretch at 1664 cm-1 suggests a protonated Schiff base linkage between the chromophore and the protein in rhodopsin as well. For comparison, this mode also appears at approximately 1660 cm-1 in both the vertebrate (bovine) and the invertebrate (octopus) rhodopsins. These data are particularly interesting since the absorption maximum of 345 nm for rhodopsin might be expected to originate from an unprotonated Schiff base linkage. That the Schiff base linkage in the owlfly rhodopsin, like in bovine and in octopus, is protonated suggests that a charged chromophore is essential to visual transduction.     

Solid-state 2H NMR spectroscopy of retinal proteins in aligned membranes

Solid-state 2H NMR spectroscopy gives a powerful avenue to investigating the structures of ligands and cofactors bound to integral membrane proteins. For bacteriorhodopsin (bR) and rhodopsin, retinal was site-specifically labeled by deuteration of the methyl groups followed by regeneration of the apoprotein. 2H NMR studies of aligned membrane samples were conducted under conditions where rotational and translational diffusion of the protein were absent on the NMR time scale. The theoretical lineshape treatment involved a static axial distribution of rotating C-C2H3 groups about the local membrane frame, together with the static axial distribution of the local normal relative to the average normal. Simulation of solid-state 2H NMR lineshapes gave both the methyl group orientations and the alignment disorder (mosaic spread) of the membrane stack. The methyl bond orientations provided the angular restraints for structural analysis. In the case of bR the retinal chromophore is nearly planar in the dark- and all-trans light-adapted states, as well upon isomerization to 13-cis in the M state. The C13-methyl group at the "business end" of the chromophore changes its orientation to the membrane upon photon absorption, moving towards W182 and thus driving the proton pump in energy conservation. Moreover, rhodopsin was studied as a prototype for G protein-coupled receptors (GPCRs) implicated in many biological responses in humans. In contrast to bR, the retinal chromophore of rhodopsin has an 11-cis conformation and is highly twisted in the dark state. Three sites of interaction affect the torsional deformation of retinal, viz. the protonated Schiff base with its carboxylate counterion; the C9-methyl group of the polyene; and the beta-ionone ring within its hydrophobic pocket. For rhodopsin, the strain energy and dynamics of retinal as established by 2H NMR are implicated in substituent control of activation. Retinal is locked in a conformation that is twisted in the direction of the photoisomerization, which explains the dark stability of rhodopsin and allows for ultra-fast isomerization upon absorption of a photon. Torsional strain is relaxed in the meta I state that precedes subsequent receptor activation. Comparison of the two retinal proteins using solid-state 2H NMR is thus illuminating in terms of their different biological functions.     

Agonist-induced conformational changes in bovine rhodopsin: insight into activation of G-protein-coupled receptors

Activation of G-protein-coupled receptors (GPCRs) is initiated by conformational changes in the transmembrane (TM) helices and the intra- and extracellular loops induced by ligand binding. Understanding the conformational changes in GPCRs leading to activation is imperative in deciphering the role of these receptors in the pathology of diseases. Since the crystal structures of activated GPCRs are not yet available, computational methods and biophysical techniques have been used to predict the structures of GPCR active states. We have recently applied the computational method LITiCon to understand the ligand-induced conformational changes in β₂-adrenergic receptor by ligands of varied efficacies. Here we report a study of the conformational changes associated with the activation of bovine rhodopsin for which the crystal structure of the inactive state is known. Starting from the inactive (dark) state, we have predicted the TM conformational changes that are induced by the isomerization of 11-cis retinal to all-trans retinal leading to the fully activated state, metarhodopsin II. The predicted active state of rhodopsin satisfies all of the 30 known experimental distance constraints. The predicted model also correlates well with the experimentally observed conformational switches in rhodopsin and other class A GPCRs, namely, the breaking of the ionic lock between R135^3.50 at the intracellular end of TM3 (part of the DRY motif) and E247^6.30 on TM6, and the rotamer toggle switch on W265^6.48 on TM6. We observe that the toggling of the W265^6.48 rotamer modulates the bend angle of TM6 around the conserved proline. The rotamer toggling is facilitated by the formation of a water wire connecting S298^7.45, W265^6.48 and H211^5.46. As a result, the intracellular ends of TMs 5 and 6 move outward from the protein core, causing large conformational changes at the cytoplasmic interface. The predicted outward movements of TM5 and TM6 are in agreement with the recently published crystal structure of opsin, which is proposed to be close to the active-state structure. In the predicted active state, several residues in the intracellular loops, such as R69, V139^3.54, T229, Q237, Q239, S240, T243 and V250^6.33, become more water exposed compared to the inactive state. These residues may be involved in mediating the conformational signal from the receptor to the G protein. From mutagenesis studies, some of these residues, such as V139^3.54, T229 and V250^6.33, are already implicated in G-protein activation. The predicted active state also leads to the formation of new stabilizing interhelical hydrogen-bond contacts, such as those between W265^6.48 and H211^5.46 and E122^3.37 and C167^4.56. These hydrogen-bond contacts serve as potential conformational switches offering new opportunities for future experimental investigations. The calculated retinal binding energy surface shows that binding of an agonist makes the receptor dynamic and flexible and accessible to many conformations, while binding of an inverse agonist traps the receptor in the inactive state and makes the other conformations inaccessible.     

Electron crystallography reveals the structure of metarhodopsin I

Rhodopsin is the prototypical G protein-coupled receptor, responsible for detection of dim light in vision. Upon absorption of a photon, rhodopsin undergoes structural changes, characterised by distinct photointermediates. Currently, only the ground-state structure has been described. We have determined a density map of a photostationary state highly enriched in metarhodopsin I, to a resolution of 5.5 A in the membrane plane, by electron crystallography. The map shows density for helix 8, the cytoplasmic loops, the extracellular plug, all tryptophan residues, an ordered cholesterol molecule and the beta-ionone ring. Comparison of this map with X-ray structures of the ground state reveals that metarhodopsin I formation does not involve large rigid-body movements of helices, but there is a rearrangement close to the bend of helix 6, at the level of the retinal chromophore. There is no gradual build-up of the large conformational change known to accompany metarhodopsin II formation. The protein remains in a conformation similar to that of the ground state until late in the photobleaching process.     

Resonance Raman studies of bovine metarhodopsin I and metarhodopsin II

The resonance Raman spectra of bovine metarhodopsin I and metarhodopsin II have been measured. The spectra are compared with model chromophore resonance Raman data. It was found that metarhodopsin I is linked to opsin via a protonated Schiff base linkage, whereas metarhodopsin II is linked by an unprotonated Schiff base. A recent suggestion that the chromophore of metarhodopsin II is retinal is explicitly disproved. The chromophores of both metarhodopsins are found to have an essentially all-trans conformation. The basic mechanism for color regulation in both forms appears to be electron delocalization. The data tend to support the model of cis-trans isomerization as the primary mechanism for vision. Also, the conclusions and inferences of this work on energy uses and storage by rhodopsin in neural generation are discussed.     

Removal of the 9-methyl group of retinal inhibits signal transduction in the visual process. A Fourier transform infrared and biochemical investigation

The photoreaction of opsin regenerated with 9-demethylretinal has been investigated by UV-vis spectroscopy, flash photolysis experiments, and Fourier transform infrared difference spectroscopy. In addition, the capability of the illuminated pigment to activate the retinal G-protein has been tested. The photoproduct, which can be stabilized at 77 K, resembles more the lumirhodopsin species, and only minor further changes occur upon warming the sample to 170 K (stabilizing lumirhodopsin). UV-vis spectroscopy reveals no further changes at 240 K (stabilizing metarhodopsin I), but infrared difference spectroscopy shows that the protein as well as the chromophore undergoes further molecular changes which are, however, different from those observed for unmodified metarhodopsin I. UV-vis spectroscopy, flash photolysis experiments, and infrared difference spectroscopy demonstrate that an intermediate different from metarhodopsin II is produced at room temperature, of which the Schiff base is still protonated. The illuminated pigment was able to activate G-protein, as assayed by monitoring the exchange of GDP for GTP gamma S in purified G-protein, only to a very limited extent (approximately 8% as compared to rhodopsin). The results are interpreted in terms of a specific steric interaction of the 9-methyl group of the retinal in rhodopsin with the protein, which is required to initiate the molecular changes necessary for G-protein activation. The residual activation suggests a conformer of the photolyzed pigment which mimics metarhodopsin II to a very limited extent.     

A spectrally silent transformation in the photolysis of octopus rhodopsin: a protein conformational change without any accompanying change of the chromophore's absorption

A spectrally silent transformation in the photolysis of octopus rhodopsin was detected by the time-resolved transient grating method. Our results showed that at least two photointermediates, which share the same chromophore absorption spectrum, exist after the final absorption changes. Previously, mesorhodopsin was thought to decay to the final photoproduct, acid metarhodopsin with a lifetime of 38 micros at 15 degrees C, but the present results show that there is at least one intermediate species (called transient acid metarhodopsin) with a lifetime of 180 micros at 15 degrees C, before forming acid metarhodopsin. This indicates that the parts of the protein distant from the chromophore are still changing even after the changes in microenvironment around the chromophore are over. From the signal intensity detected by the transient grating method, the volume change of the spectrally silent transformation was found to be DeltaV = 13 ml/mol. The activation energy of the spectrally silent transformation is much lower than those of other transformations of octopus rhodopsin. Since stable acid metarhodopsin has not been shown to activate the G protein, this transient acid metarhodopsin may be responsible for G protein activation.