Evidence for the specific interaction of a lipid molecule with rhodopsin which is altered in the transition to the active state metarhodopsin II

Rhodopsin, light-sensor of vision

The light sensor of vertebrate scotopic (low-light) vision, rhodopsin, is a G-protein-coupled receptor comprising a polypeptide chain with bound chromophore, 11-cis-retinal, that exhibits remarkable physicochemical properties. This photopigment is extremely stable in the dark, yet its chromophore isomerises upon photon absorption with 70% efficiency, enabling the activation of its G-protein, transducin, with high efficiency. Rhodopsin's photochemical and biochemical activities occur over very different time-scales: the energy of retinaldehyde's excited state is stored in <1 ps in retinal-protein interactions, but it takes milliseconds for the catalytically active state to form, and many tens of minutes for the resting state to be restored. In this review, we describe the properties of rhodopsin and its role in rod phototransduction. We first introduce rhodopsin's gross structural features, its evolution, and the basic mechanisms of its activation. We then discuss light absorption and spectral sensitivity, photoreceptor electrical responses that result from the activity of individual rhodopsin molecules, and recovery of rhodopsin and the visual system from intense bleaching exposures. We then provide a detailed examination of rhodopsin's molecular structure and function, first in its dark state, and then in the active Meta states that govern its interactions with transducin, rhodopsin kinase and arrestin. While it is clear that rhodopsin's molecular properties are exquisitely honed for phototransduction, from starlight to dawn/dusk intensity levels, our understanding of how its molecular interactions determine the properties of scotopic vision remains incomplete. We describe potential future directions of research, and outline several major problems that remain to be solved.

DEER Analysis of GPCR Conformational Heterogeneity

G protein-coupled receptors (GPCRs) represent a large class of transmembrane helical proteins which are involved in numerous physiological signaling pathways and therefore represent crucial pharmacological targets. GPCR function and the action of therapeutic molecules are defined by only a few parameters, including receptor basal activity, ligand affinity, intrinsic efficacy and signal bias. These parameters are encoded in characteristic receptor conformations existing in equilibrium and their populations, which are thus of paramount interest for the understanding of receptor (mal-)functions and rational design of improved therapeutics. To this end, the combination of site-directed spin labeling and EPR spectroscopy, in particular double electron-electron resonance (DEER), is exceedingly valuable as it has access to sub-Angstrom spatial resolution and provides a detailed picture of the number and populations of conformations in equilibrium. This review gives an overview of existing DEER studies on GPCRs with a focus on the delineation of structure/function frameworks, highlighting recent developments in data analysis and visualization. We introduce "conformational efficacy" as a parameter to describe ligand-specific shifts in the conformational equilibrium, taking into account the loose coupling between receptor segments observed for different GPCRs using DEER.

Molecular details of the unique mechanism of chloride transport by a cyanobacterial rhodopsin

Microbial rhodopsins are well known as versatile and ubiquitous light-driven ion transporters and photosensors. While the proton transport mechanism has been studied in great detail, much less is known about various modes of anion transport. Until recently, only two main groups of light-driven anion pumps were known, archaeal halorhodopsins (HRs) and bacterial chloride pumps (known as ClRs or NTQs). Last year, another group of cyanobacterial anion pumps with a very distinct primary structure was reported. Here, we studied the chloride-transporting photocycle of a representative of this new group, Mastigocladopsis repens rhodopsin (MastR), using time-resolved spectroscopy in the infrared and visible ranges and site-directed mutagenesis. We found that, in accordance with its unique amino acid sequence containing many polar residues in the transmembrane region of the protein, its photocycle features a number of unusual molecular events not known for other anion-pumping rhodopsins. It appears that light-driven chloride ion transfers by MastR are coupled with translocation of protons and water molecules as well as perturbation of several polar sidechains. Of particular interest is transient deprotonation of Asp-85, homologous to the cytoplasmic proton donor of light-driven proton pumps (such as Asp-96 of bacteriorhodopsin), which may serve as a regulatory mechanism.

Characterizing rhodopsin signaling by EPR spectroscopy: from structure to dynamics

Electron paramagnetic resonance (EPR) spectroscopy, together with spin labeling techniques, has played a major role in the characterization of rhodopsin, the photoreceptor protein and G protein-coupled receptor (GPCR) in rod cells. Two decades ago, these biophysical tools were the first to identify transmembrane helical movements in rhodopsin upon photo-activation, a critical step in the study of GPCR signaling. EPR methods were employed to identify functional loop dynamics within rhodopsin, to measure light-induced millisecond timescale changes in rhodopsin conformation, to characterize the effects of partial agonists on the apoprotein opsin, and to study lipid interactions with rhodopsin. With the emergence of advanced pulsed EPR techniques, the stage was set to determine the amplitude of structural changes in rhodopsin and the dynamics in the rhodopsin signaling complexes. Work in this area has yielded invaluable information about mechanistic properties of GPCRs. Using EPR techniques, receptors are studied in native-like membrane environments and the effects of lipids on conformational equilibria can be explored. This perspective addresses the impact of EPR methods on rhodopsin and GPCR structural biology, highlighting historical discoveries made with spin labeling techniques, and outlining exciting new directions in the field.

The Activation Pathway of Human Rhodopsin in Comparison to Bovine Rhodopsin

Rhodopsin, the photoreceptor of rod cells, absorbs light to mediate the first step of vision by activating the G protein transducin (Gt). Several human diseases, such as retinitis pigmentosa or congenital night blindness, are linked to rhodopsin malfunctions. Most of the corresponding in vivo studies and structure-function analyses (e.g. based on protein x-ray crystallography or spectroscopy) have been carried out on murine or bovine rhodopsin. Because these rhodopsins differ at several amino acid positions from human rhodopsin, we conducted a comprehensive spectroscopic characterization of human rhodopsin in combination with molecular dynamics simulations. We show by FTIR and UV-visible difference spectroscopy that the light-induced transformations of the early photointermediates are very similar. Significant differences between the pigments appear with formation of the still inactive Meta I state and the transition to active Meta II. However, the conformation of Meta II and its activity toward the G protein are essentially the same, presumably reflecting the evolutionary pressure under which the active state has developed. Altogether, our results show that although the basic activation pathways of human and bovine rhodopsin are similar, structural deviations exist in the inactive conformation and during receptor activation, even between closely related rhodopsins. These differences between the well studied bovine or murine rhodopsins and human rhodopsin have to be taken into account when the influence of point mutations on the activation pathway of human rhodopsin are investigated using the bovine or murine rhodopsin template sequences.

Modulation of the interaction between neurotensin receptor NTS1 and Gq protein by lipid

Membrane lipids have been implicated to influence the activity of G-protein-coupled receptors (GPCRs). Almost all of our knowledge on the role of lipids on GPCR and G protein function comes from work on the visual pigment rhodopsin and its G protein transducin, which reside in a highly specialized membrane environment. Thus, insight gained from rhodopsin signaling may not be simply translated to other nonvisual GPCRs. Here, we investigated the effect of lipid head group charges on the signal transduction properties of the class A GPCR neurotensin (NT) receptor 1 (NTS1) under defined experimental conditions, using self-assembled phospholipid nanodiscs prepared with the zwitter-ionic lipid 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC), the negatively charged 1-palmitoyl-2-oleoyl-sn-glycero-3-phospho-(1'-rac-glycerol) (POPG), or a POPC/POPG mixture. A combination of dynamic light scattering and sedimentation velocity showed that NTS1 was monomeric in POPC-, POPC/POPG-, and POPG-nanodiscs. Binding of the agonist NT to NTS1 occurred with similar affinities and was essentially unaffected by the phospholipid composition. In contrast, Gq protein coupling to NTS1 in various lipid nanodiscs was significantly different, and the apparent affinity of Gαq and Gβ(1)γ(1) to activated NTS1 increased with increasing POPG content. NTS1-catalyzed GDP/GTPγS nucleotide exchange at Gαq in the presence of Gβ(1)γ(1) and NT was crucially affected by the lipid type, with exchange rates higher by 1 or 2 orders of magnitude in POPC/POPG- and POPG-nanodiscs, respectively, compared to POPC-nanodiscs. Our data demonstrate that negatively charged lipids in the immediate vicinity of a nonvisual GPCR modulate the G-protein-coupling step.

Conserved Tyr223(5.58) plays different roles in the activation and G-protein interaction of rhodopsin

Rhodopsin, a seven transmembrane helix (TM) receptor, binds its ligand 11-cis-retinal via a protonated Schiff base. Coupling to the G-protein transducin (G(t)) occurs after light-induced cis/trans-retinal isomerization, which leads through photoproducts into a sequence of metarhodopsin (Meta) states: Meta I ⇌ Meta IIa ⇌ Meta IIb ⇌ Meta IIbH(+). The structural changes behind this three-step activation scheme are mediated by microswitch domains consisting of conserved amino acids. Here we focus on Tyr223(5.58) as part of the Y(5.58)X(7)K(R)(5.66) motif. Mutation to Ala, Phe, or Glu results in specific impairments of G(t)-activation measured by intrinsic G(t) fluorescence. UV-vis/FTIR spectroscopy of rhodopsin and its complex with a C-terminal G(t)α peptide allows the assignment of these deficiencies to specific steps in the activation path. Effects of mutation occur already in Meta I but do not directly influence deprotonation of the Schiff base during formation of Meta IIa. Absence of the whole phenol ring (Y223A) allows the activating motion of TM6 in Meta IIb but impairs the coupling to G(t). When only the hydroxyl group is lacking (Y223F), Meta IIb does not accumulate, but the activity toward G(t) remains substantial. From the FTIR features of Meta IIbH(+) we conclude that proton uptake to Glu134(3.49) is mandatory for Tyr223(5.58) to engage in the interaction with the key player Arg135(3.50) predicted by X-ray analysis. This polar interaction is partially recovered in Y223E, explaining its relatively high activity. Only the phenol side chain of tyrosine provides all characteristics for accumulation of the active state and G-protein activation.

Sequential rearrangement of interhelical networks upon rhodopsin activation in membranes: the Meta II(a) conformational substate

Photon absorption by rhodopsin is proposed to lead to an activation pathway that is described by the extended reaction scheme Meta I <==>Meta II(a) <==> Meta II(b) <==> Meta II(b)H(+), where Meta II(b)H(+) is thought to be the conformational substate that activates the G protein transducin. Here we test this extended scheme for rhodopsin in a membrane bilayer environment by investigating lipid perturbation of the activation mechanism. We found that symmetric membrane lipids having two unsaturated acyl chains, such as 1,2-dioleoyl-sn-glycero-3-phosphocholine (DOPC), selectively stabilize the Meta II(a) substate in the above mechanism. By combining FTIR and UV-visible difference spectroscopy, we characterized the structural and functional changes involved in the transition to the Meta II(a) intermediate, which links the inactive Meta I intermediate with the Meta II(b) states formed by helix rearrangement. Besides the opening of the Schiff base ionic lock, the Meta II(a) substate is characterized by an activation switch in a conserved water-mediated hydrogen-bonded network involving transmembrane helices H1/H2/H7, which is sensed by its key residue Asp83. On the other hand, movement of retinal toward H5 and its interaction with another interhelical H3/H5 network mediated by His211 and Glu122 is absent in Meta II(a). The latter rearrangement takes place only in the subsequent transition to Meta II(b), which has been previously associated with movement of H6. Our results imply that activating structural changes in the H1/H2/H7 network are triggered by disruption of the Schiff base salt bridge and occur prior to other chromophore-induced changes in the H3/H5 network and the outward tilt of H6 in the activation process.

New Insights into Light-Induced Deactivation of Active Rhodopsin by SVD and Global Analysis of Time-Resolved UV/Vis- and FTIR-Data

Time-resolved Fourier transform infrared (FTIR) and UV/Vis difference spectra of light induced deactivation of the photoreceptor rhodopsin were simultaneously recorded on the same sample. The data were analyzed by a special designed combination of singular value decomposition and Global analysis to verify our recently published model of receptor deactivation. This mathematical approach enables us to obtain the pure difference spectra of the conversions between the species involved. We found two different species, which could be identified as key intermediates of the model. The new data allow deeper insights into the structural changes that come along with the formation of the deactivated state. By means of this method we can now separate and assign even strongly overlapping and highly coupled bands of the infrared difference spectra.

Phospholipid meets all-trans-retinal: the making of RPE bisretinoids

The lipid phase of the photoreceptor outer segment membrane is essential to the photon capturing and signaling functions of rhodopsin. Rearrangement of phospholipids in the bilayer accompanies the formation of the active intermediates of rhodopsin following photon absorption. Furthermore, evidence for the formation of a condensation product between the photolyzed chromophore all-trans-retinal and phosphatidylethanolamine indicates that phospholipid may also participate in the movement of the retinoid in the membrane. The downside of these interactions is the formation of bisretinoid-phosphatidylethanolamine compounds that accumulate in retinal pigment epithelial cells with age and that are particularly abundant in some retinal disorders. The propensity of these compounds to negatively impact on the cells has been linked to the pathogenesis of some retinal disorders including juvenile onset recessive Stargardt disease and age-related macular degeneration.

Location of the retinal chromophore in the activated state of rhodopsin*

Rhodopsin is a highly specialized G protein-coupled receptor (GPCR) that is activated by the rapid photochemical isomerization of its covalently bound 11-cis-retinal chromophore. Using two-dimensional solid-state NMR spectroscopy, we defined the position of the retinal in the active metarhodopsin II intermediate. Distance constraints were obtained between amino acids in the retinal binding site and specific (13)C-labeled sites located on the beta-ionone ring, polyene chain, and Schiff base end of the retinal. We show that the retinal C20 methyl group rotates toward the second extracellular loop (EL2), which forms a cap on the retinal binding site in the inactive receptor. Despite the trajectory of the methyl group, we observed an increase in the C20-Gly(188) (EL2) distance consistent with an increase in separation between the retinal and EL2 upon activation. NMR distance constraints showed that the beta-ionone ring moves to a position between Met(207) and Phe(208) on transmembrane helix H5. Movement of the ring toward H5 was also reflected in increased separation between the Cepsilon carbons of Lys(296) (H7) and Met(44) (H1) and between Gly(121) (H3) and the retinal C18 methyl group. Helix-helix interactions involving the H3-H5 and H4-H5 interfaces were also found to change in the formation of metarhodopsin II reflecting increased retinal-protein interactions in the region of Glu(122) (H3) and His(211) (H5). We discuss the location of the retinal in metarhodopsin II and its interaction with sequence motifs, which are highly conserved across the pharmaceutically important class A GPCR family, with respect to the mechanism of receptor activation.

Monitoring the redox and protonation dependent contributions of cardiolipin in electrochemically induced FTIR difference spectra of the cytochrome bc(1) complex from yeast

Biochemical studies have shown that cardiolipin is essential for the integrity and activity of the cytochrome bc(1) complex and many other membrane proteins. Recently the direct involvement of a bound cardiolipin molecule (CL) for proton uptake at center N, the site of quinone reduction, was suggested on the basis of a crystallographic study. In the study presented here, we probe the low frequency infrared spectroscopy region as a technique suitable to detect the involvement of the lipids in redox induced reactions of the protein. First the individual infrared spectroscopic features of lipids, typically present in the yeast membrane, have been monitored for different pH values in micelles and vesicles. The pK(a) values for cardiolipin molecule have been observed at 4.7+/-0.3 and 7.9+/-1.3, respectively. Lipid contributions in the electrochemically induced FTIR spectra of the bc(1) complex from yeast have been identified by comparing the spectra of the as isolated form, with samples where the lipids were digested by lipase-A(2). Overall, a noteworthy perturbation in the spectral region typical for the protein backbone can be reported. Interestingly, signals at 1159, 1113, 1039 and 980 cm(-1) have shifted, indicating the perturbation of the protonation state of cardiolipin coupled to the reduction of the hemes. Additional shifts are found and are proposed to reflect lipids reorganizing due to a change in their direct environment upon the redox reaction of the hemes. In addition a small shift in the alpha band from 559 to 556 nm can be seen after lipid depletion, reflecting the interaction with heme b(H) and heme c. Thus, our work highlights the role of lipids in enzyme reactivity and structure.

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 beta(2)-adrenergic receptor.

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.

Linkage Between the Intramembrane H-bond Network Around Aspartic Acid 83 and the Cytosolic Environment of Helix 8 in Photoactivated Rhodopsin

Understanding the coupling between conformational changes in the intramembrane domain and at the membrane-exposed surface of the bovine photoreceptor rhodopsin, a prototypical G protein-coupled receptor (GPCR), is crucial for the elucidation of molecular mechanisms in GPCR activation. Here, we have combined Fourier transform infrared (FTIR) and fluorescence spectroscopy to address the coupling between conformational changes in the intramembrane region around the retinal and the environment of helix 8, a putative cytosolic surface switch region in class-I GPCRs. Using FTIR/fluorescence cross-correlation we show specifically that surface alterations monitored by emission changes of fluorescein bound to Cys316 in helix 8 of rhodopsin are highly correlated with (i) H-bonding to Asp83 proximal of the retinal Schiff base but not to Glu122 close to the beta-ionone and (ii) with a metarhodopsin II (MII)-specific 1643 cm(-1) IR absorption change, indicative of a partial loss of secondary structure in helix 8 upon MII formation. These correlations are disrupted by limited C-terminal proteolysis but are maintained upon binding of a transducin alpha-subunit (G(talpha))-derived peptide, which stabilizes the MII state. Our results suggest that additional C-terminal cytosolic loop contacts monitored by an amide II absorption at 1557 cm(-1) play a functionally crucial role in keeping helix 8 in the position in which its environment is strongly coupled to the retinal-binding site near the Schiff base. In the intramembrane region, this coupling is mediated by the H-bonding network that connects Asp83 to the NPxxY(x)F motif preceding helix 8.

How a small change in retinal leads to G-protein activation: initial events suggested by molecular dynamics calculations

Rhodopsin is the prototypical G-protein coupled receptor, coupling light activation with high efficiency to signaling molecules. The dark-state X-ray structures of the protein provide a starting point for consideration of the relaxation from initial light activation to conformational changes that may lead to signaling. In this study we create an energetically unstable retinal in the light activated state and then use molecular dynamics simulations to examine the types of compensation, relaxation, and conformational changes that occur following the cis-trans light activation. The results suggest that changes occur throughout the protein, with changes in the orientation of Helices 5 and 6, a closer interaction between Ala 169 on Helix 4 and retinal, and a shift in the Schiff base counterion that also reflects changes in sidechain interactions with the retinal. Taken together, the simulation is suggestive of the types of changes that lead from local conformational change to light-activated signaling in this prototypical system.

The all-trans-15-syn-retinal chromophore of metarhodopsin III is a partial agonist and not an inverse agonist

Meta III is formed during the decay of rhodopsin's active receptor state at neutral to alkaline pH by thermal isomerization of the retinal Schiff base C15=N bond, converting the ligand from all-trans 15-anti to all-trans 15-syn. The thereby induced change of ligand geometry switches the receptor to an inactive conformation, such that the decay pathway to Meta III contributes to the deactivation of the signaling state at higher pH values. We have examined the conformation of Meta III over a wider pH range and found that Meta III exists in a pH-dependent conformational equilibrium between this inactive conformation at neutral to alkaline pH and an active conformation similar to that of Meta II, which, however, is assumed at very acidic pH only. The apparent pKa of this transition is around 5.1 and thus several units lower than that of the Meta I/Meta II photoproduct equilibrium with its all-trans 15-anti ligand, but still about 1 unit higher than that of the opsin conformational equilibrium in the absence of ligand. The all-trans-15-syn-retinal chromophore is therefore not an inverse agonist like 11-cis- or 9-cis-retinal, which lock the receptor in an inactive conformation, but a classical partial agonist, which is capable of activating the receptor, yet with an efficiency considerably lower than the full agonist all-trans 15-anti. As the Meta III chromophore differs structurally from this full agonist only in the isomeric state of the C15=N bond, this ligand represents an excellent model system to study principal mechanisms of partial agonism which are helpful to understand the partial agonist behavior of other ligands.

G-protein coupled receptor structure

Because of their central role in regulation of cellular function, structure/function relationships for G-protein coupled receptors (GPCR) are of vital importance, yet only recently have sufficient data been obtained to begin mapping those relationships. GPCRs regulate a wide range of cellular processes, including the senses of taste, smell, and vision, and control a myriad of intracellular signaling systems in response to external stimuli. Many diseases are linked to GPCRs. A critical need exists for structural information to inform studies on mechanism of receptor action and regulation. X-ray crystal structures of only one GPCR, in an inactive state, have been obtained to date. However considerable structural information for a variety of GPCRs has been obtained using non-crystallographic approaches. This review begins with a review of the very earliest GPCR structural information, mostly derived from rhodopsin. Because of the difficulty in crystallizing GPCRs for X-ray crystallography, the extensive published work utilizing alternative approaches to GPCR structure is reviewed, including determination of three-dimensional structure from sparse constraints. The available X-ray crystallographic analyses on bovine rhodopsin are reviewed as the only available high-resolution structures for any GPCR. Structural information available on ligand binding to several receptors is included. The limited information on excited states of receptors is also reviewed. It is concluded that while considerable basic structural information has been obtained, more data are needed to describe the molecular mechanism of activation of a GPCR.

Signal Transfer from GPCRs to G Proteins

Catalysis of nucleotide exchange in heterotrimeric G proteins (Galphabetagamma) is a key step in cellular signal transduction mediated by G protein-coupled receptors. The Galpha N terminus with its helical stretch is thought to be crucial for G protein/activated receptor (R(*)) interaction. The N-terminal fatty acylation of Galpha is important for membrane targeting of G proteins. By applying biophysical techniques to the rhodopsin/transducin model system, we studied the effect of N-terminal truncations in Galpha. In Galphabetagamma, lack of the fatty acid and Galpha truncations up to 33 amino acids had little effect on R(*) binding and R(*)-catalyzed nucleotide exchange, implying that this region is not mandatory for R(*)/Galphabetagamma interaction. However, when the other hydrophobic modification of Galphabetagamma, the Ggamma C-terminal farnesyl moiety, is lacking, R(*) interaction requires the fatty acylated Galpha N terminus. This suggests that the two hydrophobic extensions can replace each other in the interaction of Galphabetagamma with R(*). We propose that in native Galphabetagamma, these two terminal regions are functionally redundant and form a microdomain that serves both to anchor the G protein to the membrane and to establish an initial docking complex with R(*). Accordingly, we find that the native fatty acylated Galpha is competent to interact with R(*) even in the absence of Gbetagamma, whereas nonacylated Galpha requires Gbetagamma for interaction. Experiments with N-terminally truncated Galpha subunits suggest that in the second step of the catalytic process, the receptor binds to the alphaN/beta1-loop region of Galpha to reduce nucleotide affinity and to make the Galpha C terminus available for subsequent interaction with R(*).

Cytoplasmic Shuttling of Protons in Anabaena Sensory Rhodopsin: Implications for Signaling Mechanism

It was found recently that Anabaena sensory rhodopsin (ASR), which possibly serves as a photoreceptor for chromatic adaptation, interacts with a soluble cytoplasmic transducer. The X-ray structure of the transducer-free protein revealed an extensive hydrogen-bonded network of amino acid residues and water molecules in the cytoplasmic half of ASR, in high contrast to its haloarchaeal counterparts. Using time-resolved spectroscopy of the wild-type and mutant ASR in the visible and infrared ranges, we tried to determine whether this hydrogen-bonded network is used to translocate protons and whether those proton transfers are important for interaction with the transducer. We found that the retinal Schiff base deprotonation, which occurs in the M intermediate of the photocycle of all-trans-ASR, results in protonation of Asp217 on the cytoplasmic side of the protein. The deprotonation of the Schiff base induces a conformational change of ASR observed through the perturbation of associated lipids. We suggest that the cytoplasmic shuttling of protons in the photocycle of all-trans-ASR and the ensuing conformational changes might activate the transducer. Consequently, the M intermediate may be the signaling state of ASR.

Location of Trp265 in metarhodopsin II: implications for the activation mechanism of the visual receptor rhodopsin

Isomerization of the 11-cis retinal chromophore in the visual pigment rhodopsin is coupled to motion of transmembrane helix H6 and receptor activation. We present solid-state magic angle spinning NMR measurements of rhodopsin and the metarhodopsin II intermediate that support the proposal that interaction of Trp265(6.48) with the retinal chromophore is responsible for stabilizing an inactive conformation in the dark, and that motion of the beta-ionone ring allows Trp265(6.48) and transmembrane helix H6 to adopt active conformations in the light. Two-dimensional dipolar-assisted rotational resonance NMR measurements are made between the C19 and C20-methyl groups of the retinal and uniformly 13C-labeled Trp265(6.48). The retinal C20-Trp265(6.48) contact present in the dark-state of rhodopsin is lost in metarhodopsin II, and a new contact is formed with the C19 methyl group. We have previously shown that the retinal translates 4-5 A toward H5 in metarhodopsin II. This motion, in conjunction with the Trp-C19 contact, implies that the Trp265(6.48) side-chain moves significantly upon rhodopsin activation. NMR measurements also show that a packing interaction in rhodopsin between Trp265(6.48) and Gly121(3.36) is lost in metarhodopsin II, consistent with H6 motion away from H3. However, a close contact between Gly120(3.35) on H3 and Met86(2.53) on H2 is observed in both rhodopsin and metarhodopsin II, suggesting that H3 does not change orientation significantly upon receptor activation.

Monitoring redox-dependent contribution of lipids in Fourier transform infrared difference spectra of complex I fromEscherichia coli

Biochemical and crystallographic studies have shown that phospholipids are essential for the integrity and activity of membrane proteins. In the study presented here, we use electrochemically induced Fourier transform infrared (FTIR) spectroscopy to demonstrate variations occurring upon the presence and absence of lipids in NADH:ubiquinone oxidoreductase (complex I) from Escherchia coli by following the C=O vibration of the lipid molecule. Complex I is activated in the presence of lipids. Interestingly, in electrochemically induced FTIR difference spectra of complex I from E. coli, a new signal at 1744/1730 cm(-1) appears after addition of E. coli polar lipids, concomitant with the oxidized or reduced form, respectively. Absorbance spectra of liposomes from mixed lipids at different pH values demonstrate shifts for the carbonyl vibration depending on the environment. On this basis we suggest that lipids, though not redox active themselves, contribute in reaction-induced FTIR difference spectra, if a change occurs in the direct environment of the lipid during the observed reaction or coupled processes.

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.

Design and synthesis of artificial phospholipid for selective cleavage of integral membrane protein

An artificial phospholipid, possessing saturated alkyl chains as a membrane anchor and protein recognition site as well as an Fe(III)-EDTA moiety as a protein cleavable polar head group, was designed and synthesized based on the amidite method for the purpose of examination of cleavage of integral membrane proteins.

Structural studies of the putative helix 8 in the human beta(2) adrenergic receptor: an NMR study

The recently reported crystal structure of bovine rhodopsin revealed a cytoplasmic helix (helix 8) in addition to the seven transmembrane helices. This domain is roughly perpendicular to the transmembrane bundle in the presence of an interface and may be a loop-like structure in the absence of an interface. Several studies carried out on this domain suggested that it might act as a conformational switch between the inactive and activated states of this G-protein coupled receptor (GPCR). These results raised the question whether helix 8 may be an important feature of other GPCRs as well. To explore this question, we determined the structure of a peptide representing the putative helix 8 domain in another receptor that belongs to the rhodopsin family of GPCRs, the human beta(2) adrenergic receptor (hbeta(2)AR), using two-dimensional (1)H nuclear magnetic resonance (NMR). The key results from this structural study are that the putative helix 8 domain is helical in detergent and in DMSO while in water this region is disordered; the conformation is therefore dependent upon the environment. Comparison of data from five GPCRs suggests that these observations may be generally important for GPCR structure and function.

Molecular Dynamics Simulation of Dark-adapted Rhodopsin in an Explicit Membrane Bilayer: Coupling between Local Retinal and Larger Scale Conformational Change

The light-driven photocycle of rhodopsin begins the photoreceptor cascade that underlies visual response. In a sequence of events, the retinal covalently attached to the rhodopsin protein undergoes a conformational change that communicates local changes to a global conformational change throughout the whole protein. In turn, the large-scale protein change then activates G-proteins and signal amplification throughout the cell. The nature of this change, involving a coupling between a local process and larger changes throughout the protein, may be important for many membrane proteins. In addition, functional work has shown that this coupling occurs with different efficiency in different lipid settings. To begin to understand the nature of the efficiency of this coupling in different lipid settings, we present a molecular dynamics study of rhodopsin in an explicit dioleoyl-phosphatidylcholine bilayer. Our system was simulated for 40 ns and provides insights into the very early events of the visual cascade, before the full transition and activation have occurred. In particular, we see an event near 10 ns that begins with a change in hydrogen bonding near the retinal and that leads through a series of coupled changes to a shift in helical tilt. This type of event, though rare on the molecular dynamics time-scale, could be an important clue to the types of coupling that occur between local and large-scale conformational change in many membrane proteins.

Spectroscopic evidence for a preferential location of lidocaine inside phospholipid bilayers

We examined the effect of uncharged lidocaine on the structure and dynamics of egg phosphatidylcholine (EPC) membranes at pH 10.5 in order to assess the location of this local anesthetic in the bilayer. Changes in the organization of small unilamellar vesicles were monitored either by electron paramagnetic resonance (EPR)-in the spectra of doxyl derivatives of stearic acid methyl esters labeled at different positions in the acyl chain (5-, 7-, 12- and 16-MeSL)-or by fluorescence, with pyrene fatty-acid (4-, 6-, 10- and 16-Py) probes. The largest effects were observed with labels located at the upper positions of the fatty-acid acyl-chain. Dynamic information was obtained by 1H-NMR. Lidocaine protons presented shorter longitudinal relaxation times (T(1)) values due to their binding, and consequent immobilization to the membrane. In the presence of lidocaine the mobility of all glycerol protons of EPC decreased, while the choline protons revealed a higher degree of mobility, indicating a reduced participation in lipid-lipid interactions. Two-dimensional Nuclear Overhauser Effect experiments detected contacts between aromatic lidocaine protons and the phospholipid-choline methyl group. Fourier-transform infrared spectroscopy spectra revealed that lidocaine changes the access of water to the glycerol region of the bilayer. A "transient site" model for lidocaine preferential location in EPC bilayers is proposed. The model is based on the consideration that insertion of the bulky aromatic ring of the anesthetic into the glycerol backbone region causes a decrease in the mobility of that EPC region (T(1) data) and an increased mobility of the acyl chains (EPR and fluorescence data).

Rhodopsin: insights from recent structural studies

The recent report of the crystal structure of rhodopsin provides insights concerning structure-activity relationships in visual pigments and related G protein-coupled receptors (GPCRs). The seven transmembrane helices of rhodopsin are interrupted or kinked at multiple sites. An extensive network of interhelical interactions stabilizes the ground state of the receptor. The ligand-binding pocket of rhodopsin is remarkably compact, and several chromophore-protein interactions were not predicted from mutagenesis or spectroscopic studies. The helix movement model of receptor activation, which likely applies to all GPCRs of the rhodopsin family, is supported by several structural elements that suggest how light-induced conformational changes in the ligand-binding pocket are transmitted to the cytoplasmic surface. The cytoplasmic domain of the receptor includes a helical domain extending from the seventh transmembrane segment parallel to the bilayer surface. The cytoplasmic surface appears to be approximately large enough to bind to the transducin heterotrimer in a one-to-one complex. The structural basis for several unique biophysical properties of rhodopsin, including its extremely low dark noise level and high quantum efficiency, can now be addressed using a combination of structural biology and various spectroscopic methods. Future high-resolution structural studies of rhodopsin and other GPCRs will form the basis to elucidate the detailed molecular mechanism of GPCR-mediated signal transduction.

Evidence that helix 8 of rhodopsin acts as a membrane-dependent conformational switch

The crystal structure of rhodopsin revealed a cytoplasmic helical segment (H8) extending from transmembrane (TM) helix seven to a pair of vicinal palmitoylated cysteine residues. We studied the structure of model peptides corresponding to H8 under a variety of conditions using steady-state fluorescence, fluorescence anisotropy, and circular dichroism spectroscopy. We find that H8 acts as a membrane-surface recognition domain, which adopts a helical structure only in the presence of membranes or membrane mimetics. The secondary structural properties of H8 further depend on membrane lipid composition with phosphatidylserine inducing helical structure. Fluorescence quenching experiments using brominated acyl chain phospholipids and vesicle leakage assays suggest that H8 lies within the membrane interfacial region where amino acid side chains can interact with phospholipid headgroups. We conclude that H8 in rhodopsin, in addition to its role in binding the G protein transducin, acts as a membrane-dependent conformational switch domain.

The amino terminus of opsin translocates "posttranslationally" as efficiently as cotranslationally

Opsin, a member of the G-protein-coupled receptor family, is a polytopic membrane protein that does not encode a cleaved amino-terminal signal sequence. The amino terminus of opsin precedes the first known targeting information, suggesting that it translocates across the endoplasmic reticulum (ER) membrane after synthesis, uncoupled from translation. However, translocation across the mammalian ER is believed to be coupled to protein synthesis. In this study we show that opsin, within a range of nascent peptide lengths, targets and translocates equally efficiently co- and posttranslationally. Longer nascent opsin peptides have a lower efficiency of cotranslational translocation but an even lower efficiency of posttranslational translocation. We also show that SRP is required for both co- and posttranslational targeting.

Structure of rhodopsin and the superfamily of seven-helical receptors: the same and not the same

The crystal structure of rhodopsin provides significant insights concerning structure/activity relationships in visual pigments and related G-protein-coupled receptors. The specific arrangement of seven-transmembrane helices is stabilized by a series of intermolecular interactions that appear to be conserved among Family A receptors. However, the potential for structural and functional diversity among members of the superfamily of seven-helical receptors presents a significant future challenge.

Conformation and stability of alpha-helical membrane proteins. 2. Influence of pH and salts on stability and unfolding of rhodopsin

We studied the stability and pH-induced denaturation of rhodopsin and its photoproducts as a model for alpha-helical membrane proteins. The increased stability of the dark state of rhodopsin as compared to its photoproduct states allows the initiation of unfolding of the protein by light-dependent isomerization of the chromophore. We could therefore characterize the transition from the native to either acid or alkaline denatured states by light-induced Fourier transform infrared difference spectroscopy, UV-visible spectroscopy, and intrinsic tryptophan fluorescence spectroscopy. The results indicate a loss of important tertiary interactions within the protein and between the protein and the retinal chromophore in the denatured state, despite that the secondary structure of the protein is almost fully retained during the transition. We therefore propose that in this denatured state the protein adopts the conformation of a loose bundle of preserved, but only weakly interacting, transmembrane helices with a largely des-oriented and partly solvent-exposed chromophore. We further characterized the influence of salts on the stability of the rhodopsin helix bundle, which was found to follow the Hofmeister series. We found that the effect of sodium chloride may be stabilizing or destabilizing, depending on the intrinsic stability of the examined protein conformation and on salt concentration. In particular, sodium chloride is shown to counteract the formation of the denatured loose bundle state presumably by increasing the lateral pressure on the helix bundle, thereby stabilizing native-like tertiary contacts within the protein.

Rhodopsin: structural basis of molecular physiology

The crystal structure of rod cell visual pigment rhodopsin was recently solved at 2.8-A resolution. A critical evaluation of a decade of structure-function studies is now possible. It is also possible to begin to explain the structural basis for several unique physiological properties of the vertebrate visual system, including extremely low dark noise levels as well as high gain and color detection. The ligand-binding pocket of rhodopsin is remarkably compact, and several apparent chromophore-protein interactions were not predicted from extensive mutagenesis or spectroscopic studies. The transmembrane helices are interrupted or kinked at multiple sites. An extensive network of interhelical interactions stabilizes the ground state of the receptor. The helix movement model of receptor activation, which might apply to all G protein-coupled receptors (GPCRs) of the rhodopsin family, is supported by several structural elements that suggest how light-induced conformational changes in the ligand-binding pocket are transmitted to the cytoplasmic surface. The cytoplasmic domain of the receptor is remarkable for a carboxy-terminal helical domain extending from the seventh transmembrane segment parallel to the bilayer surface. Thus the cytoplasmic surface appears to be approximately the right size to bind to the transducin heterotrimer in a one-to-one complex. Future high-resolution structural studies of rhodopsin and other GPCRs will form a basis to elucidate the detailed molecular mechanism of GPCR-mediated signal transduction.

A structural role for Asp83 in the photoactivation of rhodopsin

Asp83 is a highly conserved residue in the second transmembrane domain of visual pigments and many members of other G protein-coupled receptor subfamilies. Upon illumination, the rod visual pigment rhodopsin proceeds through various intermediate states (Batho<-->BSI<-->Lumi<-->Meta I<-->Meta II). Meta II represents the active state of rhodopsin, which binds and activates the G protein transducin. Evidence has been presented that Asp83 participates in the formation of Meta II and undergoes a change in H-bonding. To investigate whether this role of Asp83 requires its proton-donating capacity and/or its H-bonding capability, we constructed the mutants D83C and D83N. Both mutants appear to effectively activate transducin, indicating that Asp83 is not essential for signal transduction. Differential effects of the mutations D83C and D83N are observed in the spectral properties and the pH sensitivity of the Meta I-->Meta II transition. In general, D83C behaves much more like wild-type than D83N. We conclude that the structural role of Asp83 also involves the acidic nature of its carboxyl group. In addition, the participation in Meta II formation of Cys83 in D83C manifests itself as a change in the vibrational properties of the sulfhydryl group, demonstrating that the -SH group can be used as a non-invasive probe for local structural changes.

The photobleaching sequence of a short-wavelength visual pigment

The photobleaching pathway of a short-wavelength cone opsin purified in delipidated form (lambda(max) = 425 nm) is reported. The batho intermediate of the violet cone opsin generated at 45 K has an absorption maximum at 450 nm. The batho intermediate thermally decays to the lumi intermediate (lambda(max) = 435 nm) at 200 K. The lumi intermediate decays to the meta I (lambda(max) = 420 nm) and meta II (lambda(max) = 388 nm) intermediates at 258 and 263 K, respectively. The meta II intermediate decays to free retinal and opsin at >270 K. At 45, 75, and 140 K, the photochemical excitation of the violet cone opsin at 425 nm generates the batho intermediate at high concentrations under moderate illumination. The batho intermediate spectra, generated via decomposing the photostationary state spectra at 45 and 140 K, are identical and have properties typical of batho intermediates of other visual pigments. Extended illumination of the violet cone opsin at 75 K, however, generates a red-shifted photostationary state (relative to both the dark and the batho intermediates) that has as absorption maximum at approximately 470 nm, and thermally reverts to form the normal batho intermediate when warmed to 140 K. We conclude that this red-shifted photostationary state is a metastable state, characterized by a higher-energy protein conformation that allows relaxation of the all-trans chromophore into a more planar conformation. FTIR spectroscopy of violet cone opsin indicates conclusively that the chromophore is protonated. A similar transformation of the rhodopsin binding site generates a model for the VCOP binding site that predicts roughly 75% of the observed blue shift of the violet cone pigment relative to rhodopsin. MNDO-PSDCI calculations indicate that secondary interactions involving the binding site residues are as important as the first-order chromophore protein interactions in mediating the wavelength maximum.

Light-induced reorganization of phospholipids in rod disc membranes

The transbilayer redistribution of spin-labeled phospholipid analogues (SL-PL) with choline, serine, and ethanolamine head groups (PC, PS, and PE, respectively) was studied on intact disc vesicles of bovine rod outer segment membranes in the dark and after illumination. Redistribution was measured by the extraction of spin-labeled lipid analogues from the outer leaflet of membrane using the bovine serum albumin back-exchange assay. In the dark, PS was distributed asymmetrically, favoring the outer leaflet, whereas PC and PE showed small if any asymmetry. Green illumination for 1 min caused lipid head group-specific reorganization of SL-PL. Extraction of SL-PS by bovine serum albumin showed a fast transient (<10 min) enhancement, which was further augmented by a peptide stabilizing the active metarhodopsin II conformation. The data suggest a direct release of 1 molecule of bound PS per rhodopsin into the outer leaflet and subsequent redistribution between the two leaflets. SL-PE and SL-PC showed more complex kinetics, in both cases consistent with a prolonged period of reduced extraction (2 phospholipids per rhodopsin in each case). The different phases of SL-PL reorganization after illumination may be related to the formation and decay of the active rhodopsin species and to their subsequent regeneration process.

Rhodopsin activation affects the environment of specific neighboring phospholipids: an FTIR spectroscopic study

Rhodopsin is a member of a superfamily of G-protein-coupled receptors that transduce signals across membranes. We used Fourier-transform infrared (FTIR) difference spectroscopy to study the interaction between rhodopsin and lipid bilayer upon receptor activation. A difference band at 1744 cm(-1) (+)/1727 cm(-1) (-) was identified in the FTIR-difference spectrum of rhodopsin mutant D83N/E122Q in which spectral difference bands arising from the carbonyl stretching frequencies of protonated carboxylic acid groups were removed by mutation. As the band was abolished by detergent delipidation, we suggested that it arose from carbonyl groups of phospholipid fatty acid esters. Rhodopsin and the D83N/E122Q mutant were reconstituted into various (13)C-labeled 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine vesicles and probed. The 1744-cm(-1) (+)/1727 cm(-1) (-) band could be unequivocally assigned to a change in the lipid ester carbonyl stretch upon receptor activation, with roughly equal contribution from both lipid esters. The band intensity scaled with the amount of rhodopsin but not with the amount of lipid, excluding the possibility that it was due to the bulk lipid phase. We also excluded the possibility that the lipid band represents a change in the number of boundary lipids or a general alteration in the boundary lipid environment upon formation of metarhodopsin II. Instead, the data suggest that the lipid band represents the change of a specific lipid-receptor interaction that is coupled to protein conformational changes.

Transducin-dependent protonation of glutamic acid 134 in rhodopsin

A highly conserved carboxylic acid residue in rhodopsin, Glu(134), modulates transducin (G(t)) interaction. It has been postulated that Glu(134) becomes protonated upon receptor activation. We studied the interaction between rhodopsin and G(t) using Fourier transform infrared (FTIR) difference spectroscopy combined with attenuated total reflection (ATR). Formation of the complex between G(t) and photoactivated rhodopsin reconstituted into phosphatidylcholine vesicles caused prominent infrared absorption increases at 1641, 1550, and 1517 cm(-)(1). The rhodopsin mutant E134Q was also studied. When measured in the presence of G(t), replacement of Glu(134) by glutamine abolished the low-frequency part of a broad absorption band at 1735 cm(-)(1) that is normally superimposed on the light-induced absorption changes of Asp(83) and Glu(122) of rhodopsin. In addition, a negative absorption band at 1400 cm(-)(1) that is evoked by interaction of native metarhodopsin II (MII) with G(t) was not observed in the difference spectrum of the E134Q mutant. Thus, Glu(134) is ionized in the dark and exhibits a symmetrical COO(-) stretching vibration at 1400 cm(-)(1). Glu(134) becomes protonated in the G(t)-MII complex and displays a C=O stretching mode near 1730 cm(-)(1). The E134Q mutation also affects absorption changes attributable to lipids, suggesting that the protonation of Glu(134) is linked to transfer of the carboxylic acid side chain from a polar to a nonpolar environment by becoming exposed to the lipid phase when G(t) binds. These results show directly that Glu(134) becomes protonated in MII upon G(t) binding and suggest that changes in receptor conformation affect lipid-protein interactions.

The molecular origin of the inhibition of transducin activation in rhodopsin lacking the 9-methyl group of the retinal chromophore: a UV-Vis and FTIR spectroscopic study

The formation of the active rhodopsin state metarhodopsin II (MII) is believed to be partially governed by specific steric constraints imposed onto the protein by the 9-methyl group of the retinal chromophore. We studied the properties of the synthetic pigment 9-demethyl rhodopsin (9dm-Rho), consisting of the rhodopsin apoprotein regenerated with synthetic retinal lacking the 9-methyl group, by UV-vis and Fourier transform infrared difference spectroscopy. Low activation rates of the visual G-protein transducin by the modified pigment reported in previous studies are shown to not be caused by the reduced activity of its MII state, but to be due to a dramatic equilibrium shift from MII to its immediate precursor, MI. The MII state of 9dm-Rho displays only a partial deprotonation of the retinal Schiff base, leading to the formation of two MII subspecies absorbing at 380 and 470 nm, both of which seem to be involved in transducin activation. The rate of MII formation is slowed by 2 orders of magnitude compared to rhodopsin. The dark state and the MI state of 9dm-Rho are distinctly different from their respective states in the native pigment, pointing to a more relaxed fit of the retinal chromophore in its binding pocket. The shifted equilibrium between MI and MII is therefore discussed in terms of an increased entropy of the 9dm-Rho MI state due to changed steric interactions.