Single-Molecule Observation of the Ligand-Induced Population Shift of Rhodopsin,A G-Protein-Coupled Receptor

Rhodopsin is a G-protein-coupled receptor, in which retinal chromophore acts as inverse-agonist or agonist depending on its configuration and protonation state. Photostimulation of rhodopsin results in a pH-dependent equilibrium between the active state (Meta-II) and its inactive precursor (Meta-I). Here, we monitored conformational changes of rhodopsin using a fluorescent probe Alexa594 at the cytoplasmic surface, which shows fluorescence increase upon the generation of active state, by single-molecule measurements. The fluorescence intensity of a single photoactivated rhodopsin molecule alternated between two states. Interestingly, such a fluorescence alternation was also observed for ligand-free rhodopsin (opsin), but not for dark-state rhodopsin. In addition, the pH-dependences of Meta-I/Meta-II equilibrium estimated by fluorescence measurements deviated notably from estimates based on absorption spectra, indicating that both Meta-I and Meta-II are mixtures of two conformers. Our observations indicate that rhodopsin molecules intrinsically adopt both active and inactive conformations, and the ligand retinal shifts the conformational equilibrium. These findings provide dynamical insights into the activation mechanisms of G-protein-coupled receptors.     

Retinal Flip in Rhodopsin Activation?

Rhodopsin is a well-characterized structural model of a G protein-coupled receptor. Photoisomerization of the covalently bound retinal triggers activation. Surprisingly, the x-ray crystal structure of the active Meta-II state has a 180° rotation about the long-axis of the retinal polyene chain. Unbiased microsecond-timescale all-atom molecular dynamics simulations show that the retinal cofactor can flip back to the orientation observed in the inactive state of rhodopsin under conditions favoring the Meta-I state. Our results provide, to our knowledge, the first evidence from molecular dynamics simulations showing how rotation of the retinal ligand within its binding pocket can occur in the activation mechanism of rhodopsin.     

Rod Visual Pigment Optimizes Active State to Achieve Efficient G Protein Activation as Compared with Cone Visual Pigments

Most vertebrate retinas contain two types of photoreceptor cells, rods and cones, which show different photoresponses to mediate scotopic and photopic vision, respectively. These cells contain different types of visual pigments, rhodopsin and cone visual pigments, respectively, but little is known about the molecular properties of cone visual pigments under physiological conditions, making it difficult to link the molecular properties of rhodopsin and cone visual pigments with the differences in photoresponse between rods and cones. Here we prepared bovine and mouse rhodopsin (bvRh and mRh) and chicken and mouse green-sensitive cone visual pigments (cG and mG) embedded in nanodiscs and applied time-resolved fluorescence spectroscopy to compare their G_t activation efficiencies. Rhodopsin exhibited greater G_t activation efficiencies than cone visual pigments. Especially, the G_t activation efficiency of mRh was about 2.5-fold greater than that of mG at 37 °C, which is consistent with our previous electrophysiological data of knock-in mice. Although the active state (Meta-II) was in equilibrium with inactive states (Meta-I and Meta-III), quantitative determination of Meta-II in the equilibrium showed that the G_t activation efficiency per Meta-II of bvRh was also greater than those of cG and mG. These results indicated that efficient G_t activation by rhodopsin, resulting from an optimized active state of rhodopsin, is one of the causes of the high amplification efficiency of rods.     

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

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

Molecular dynamics simulation of dark-adapted rhodopsin and free opsin

Molecular dynamics simulation was carried out for the rhodopsin protein to investigate its conformational changes in respect to inclusion of 11-cis retinal chromophore. Molecular dynamics calculations were performed within the time frame 3000 ps. Totally, 3 X 10(6) configurations ofrhodopsin and free opsin were analyzed and compared. It has been shown that the 11-cis retinal rearrangement (adaptation) in opsin strongly affects the surrounding amino acid residues of protein binding pocket and the protein cytoplasmic region. The extracellular part, however, shows comparatively little changes. On basis of the simulation results obtained we propose a molecular mechanism for the rhodopsin protein function as a G-protein-coupled receptor in the state of darkness. We discuss the role of the retinal chromophore as a ligand-antagonist stabilizing the inactive conformation of rhodopsin.     

Conformations of the active and inactive states of opsin

The signaling state metarhodopsin II of the visual pigment rhodopsin decays to the apoprotein opsin and all-trans retinal, which are then regenerated to rhodopsin by the visual cycle. Opsin is known to have at neutral pH only a small residual constitutive activity toward its G protein transducin, which is thought to play a considerable role in light adaptation (bleaching desensitization). In this study we show with Fourier-transform infrared spectroscopy that after metarhodopsin II decay, opsin exists in two conformational states that are in a pH-dependent equilibrium at 30 degrees C with a pK of 4.1 in the presence of hydroxylamine scavenging the endogenous all-trans retinal. Despite the lack of the native agonist in its binding pocket, the low pH opsin conformation is very similar to that of metarhodopsin II and is likewise stabilized by peptides derived from rhodopsin's cognate G protein, transducin. The high pH form, on the other hand, has some conformational similarity to the inactive metarhodopsin I state. We therefore conclude that the opsin apoprotein displays intrinsic conformational states that are merely modulated by bound all-trans retinal.     

Elucidation of the nature of the conformational changes of the EF-interhelical loop in bacteriorhodopsin and of the helix VIII on the cytoplasmic surface of bovine rhodopsin: a time-resolved fluorescence depolarization study

The conformation of the AB-loop and EF-loop of bacteriorhodopsin and of the fourth cytoplasmic loop (helix VIII) of bovine rhodopsin were assessed by a combination of time-resolved fluorescence depolarization and site-directed fluorescence labeling. The fluorescence anisotropy decays were measured employing a tunable Ti:sapphire laser/microchannel plate based single-photon counting apparatus with picosecond time resolution. This method allows measurement of the diffusional dynamics of the loops directly on a nanosecond time-scale. We implemented the method to study model peptides and two-helix systems representing sequences of bacteriorhodopsin. Thus, we systematically analyzed the anisotropic behavior of four different fluorescent dyes covalently bound to a single cysteine residue on the protein surface and assigned the anisotropy decay components to the modes of motion of the protein and its segments. We have identified two mechanisms of loop conformational changes in the functionally intact proteins bacteriorhodopsin and bovine rhodopsin. First, we found a surface potential-dependent transition between two conformational states of the EF-loop of bacteriorhodopsin, detected with the fluorescent dye bound to position 160. A transition between the two conformational states at 150mM KCl and 20 degrees C requires a surface potential change that corresponds to Deltasigma approximately -1.0e(-)/bacteriorhodopsin molecule. We suggest, that the surface potential-based switch of the EF-loop is the missing link between the movement of helix F and the transient surface potential change detected during the photocycle of bacteriorhodopsin. Second, in the visual pigment rhodopsin, with the fluorescent dye bound to position 316, a particularly striking pH-dependent conformational change of the fourth loop on the cytoplasmic surface was analyzed. The loop mobility increased from pH 5 to 8. The midpoint of this transition is at pH 6.2 and correlates with the midpoint of the pH-dependent equilibrium between the active metarhodopsin II and the inactive metarhodopsin I state.     

Putative Active States of a Prototypic G-Protein-Coupled Receptor from Biased Molecular Dynamics

A major current focus of structural work on G-protein-coupled receptors (GPCRs) pertains to the investigation of their active states. However, for virtually all GPCRs, active agonist-bound intermediate states have been difficult to characterize experimentally owing to their higher conformational flexibility, and thus intrinsic instability, as compared to inactive inverse agonist-bound states. In this work, we explored possible activation pathways of the prototypic GPCR bovine rhodopsin by means of biased molecular dynamics simulations. Specifically, we used an explicit atomistic representation of the receptor and its environment, and sampled the conformational transition from the crystal structure of a photoactivated deprotonated state of rhodopsin to the low pH crystal structure of opsin in the presence of 11-trans-retinal, using adiabatic biased molecular dynamics simulations. We then reconstructed the system free-energy landscape along the predetermined transition trajectories using a path collective variable approach based on metadynamics. Our results suggest that the two experimental endpoints of rhodopsin/opsin are connected by at least two different pathways, and that the conformational transition is populated by at least four metastable states of the receptor, characterized by a different amplitude of the outward movement of transmembrane helix 6.     

Membrane Curvature Revisited—the Archetype of Rhodopsin Studied by Time-Resolved Electronic Spectroscopy

G-protein-coupled receptors (GPCRs) comprise the largest and most pharmacologically targeted membrane protein family. Here, we used the visual receptor rhodopsin as an archetype for understanding membrane lipid influences on conformational changes involved in GPCR activation. Visual rhodopsin was recombined with lipids varying in their degree of acyl chain unsaturation and polar headgroup size using 1-palmitoyl-2-oleoyl-sn-glycero- and 1,2-dioleoyl-sn-glycerophospholipids with phosphocholine (PC) or phosphoethanolamine (PE) substituents. The receptor activation profile after light excitation was measured using time-resolved ultraviolet-visible spectroscopy. We discovered that more saturated POPC lipids back shifted the equilibrium to the inactive state, whereas the small-headgroup, highly unsaturated DOPE lipids favored the active state. Increasing unsaturation and decreasing headgroup size have similar effects that combine to yield control of rhodopsin activation, and necessitate factors beyond proteolipid solvation energy and bilayer surface electrostatics. Hence, we consider a balance of curvature free energy with hydrophobic matching and demonstrate how our data support a flexible surface model (FSM) for the coupling between proteins and lipids. The FSM is based on the Helfrich formulation of membrane bending energy as we previously first applied to lipid-protein interactions. Membrane elasticity and curvature strain are induced by lateral pressure imbalances between the constituent lipids and drive key physiological processes at the membrane level. Spontaneous negative monolayer curvature toward water is mediated by unsaturated, small-headgroup lipids and couples directly to GPCR activation upon light absorption by rhodopsin. For the first time to our knowledge, we demonstrate this modulation in both the equilibrium and pre-equilibrium evolving states using a time-resolved approach.     

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.     

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.     

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.     

Salt effects on the conformational stability of the visual G-protein-coupled receptor rhodopsin

Membrane protein stability is a key parameter with important physiological and practical implications. Inorganic salts affect protein stability, but the mechanisms of their interactions with membrane proteins are not completely understood. We have undertaken the study of a prototypical G-protein-coupled receptor, the α-helical membrane protein rhodopsin from vertebrate retina, and explored the effects of inorganic salts on the thermal decay properties of both its inactive and photoactivated states. Under high salt concentrations, rhodopsin significantly increased its activation enthalpy change for thermal bleaching, whereas acid denaturation affected the formation of a denatured loose-bundle state for both the active and inactive conformations. This behavior seems to correlate with changes in protonated Schiff-base hydrolysis. However, chromophore regeneration with the 11-cis-retinal chromophore and MetarhodopsinII decay kinetics were slower only in the presence of sodium chloride, suggesting that in this case, the underlying phenomenon may be linked to the activation of rhodopsin and the retinal release processes. Furthermore, the melting temperature, determined by means of circular dichroism and differential scanning calorimetry measurements, was increased in the presence of high salt concentrations. The observed effects on rhodopsin could indicate that salts favor electrostatic interactions in the retinal binding pocket and indirectly favor hydrophobic interactions at the membrane protein receptor core. These effects can be exploited in applications where the stability of membrane proteins in solution is highly desirable.     

Structural insights into G-protein-coupled receptor activation

G-protein-coupled receptors (GPCRs) are the largest family of eukaryotic plasma membrane receptors, and are responsible for the majority of cellular responses to external signals. GPCRs share a common architecture comprising seven transmembrane (TM) helices. Binding of an activating ligand enables the receptor to catalyze the exchange of GTP for GDP in a heterotrimeric G protein. GPCRs are in a conformational equilibrium between inactive and activating states. Crystallographic and spectroscopic studies of the visual pigment rhodopsin and two beta-adrenergic receptors have defined some of the conformational changes associated with activation.     

The Two-Photon Reversible Reaction of the Bistable Jumping Spider Rhodopsin-1

Bistable opsins are photopigments expressed in both invertebrates and vertebrates. These light-sensitive G-protein-coupled receptors undergo a reversible reaction upon illumination. A first photon initiates the cis to trans isomerization of the retinal chromophore—attached to the protein through a protonated Schiff base—and a series of transition states that eventually results in the formation of the thermally stable and active Meta state. Excitation by a second photon reverts this process to recover the original ground state. On the other hand, monostable opsins (e.g., bovine rhodopsin) lose their chromophore during the decay of the Meta II state (i.e., they bleach). Spectroscopic studies on the molecular details of the two-photon cycle in bistable opsins are limited. Here, we describe the successful expression and purification of recombinant rhodopsin-1 from the jumping spider Hasarius adansoni (JSR1). In its natural configuration, spectroscopic characterization of JSR1 is hampered by the similar absorption spectra in the visible spectrum of the inactive and active states. We solved this issue by separating their absorption spectra by replacing the endogenous 11-cis retinal chromophore with the blue-shifted 9-cis JSiR1. With this system, we used time-resolved ultraviolet-visible spectroscopy after pulsed laser excitation to obtain kinetic details of the rise and decay of the photocycle intermediates. We also used resonance Raman spectroscopy to elucidate structural changes of the retinal chromophore upon illumination. Our data clearly indicate that the protonated Schiff base is stable throughout the entire photoreaction. We additionally show that the accompanying conformational changes in the protein are different from those of monostable rhodopsin, as recorded by light-induced FTIR difference spectroscopy. Thus, we envisage JSR1 as becoming a model system for future studies on the reaction mechanisms of bistable opsins, e.g., by time-resolved x-ray crystallography.     

Human Blue Cone Opsin Regeneration Involves Secondary Retinal Binding with Analog Specificity

Human color vision is mediated by the red, green, and blue cone visual pigments. Cone opsins are G-protein-coupled receptors consisting of an opsin apoprotein covalently linked to the 11-cis-retinal chromophore. All visual pigments share a common evolutionary origin, and red and green cone opsins exhibit a higher homology, whereas blue cone opsin shows more resemblance to the dim light receptor rhodopsin. Here we show that chromophore regeneration in photoactivated blue cone opsin exhibits intermediate transient conformations and a secondary retinoid binding event with slower binding kinetics. We also detected a fine-tuning of the conformational change in the photoactivated blue cone opsin binding site that alters the retinal isomer binding specificity. Furthermore, the molecular models of active and inactive blue cone opsins show specific molecular interactions in the retinal binding site that are not present in other opsins. These findings highlight the differential conformational versatility of human cone opsin pigments in the chromophore regeneration process, particularly compared to rhodopsin, and point to relevant functional, unexpected roles other than spectral tuning for the cone visual pigments.     

Preferential binding of allosteric modulators to active and inactive conformational states of metabotropic glutamate receptors

Metabotropic glutamate receptors (mGluRs) are G protein coupled receptors that play important roles in synaptic plasticity and other neuro-physiological and pathological processes. Allosteric mGluR ligands are particularly promising drug targets because of their modulatory effects--enhancing or suppressing the response of mGluRs to glutamate. The mechanism by which this modulation occurs is not known. Here, we propose the hypothesis that positive and negative modulators will differentially stabilize the active and inactive conformations of the receptors, respectively. To test this hypothesis, we have generated computational models of the transmembrane regions of different mGluR subtypes in two different conformations. The inactive conformation was modeled using the crystal structure of the inactive, dark state of rhodopsin as template and the active conformation was created based on a recent model of the light-activated state of rhodopsin. Ligands for which the nature of their allosteric effects on mGluRs is experimentally known were docked to the modeled mGluR structures using ArgusLab and Autodock softwares. We find that the allosteric ligand binding pockets of mGluRs are overlapping with the retinal binding pocket of rhodopsin, and that ligands have strong preferences for the active and inactive states depending on their modulatory nature. In 8 out of 14 cases (57%), the negative modulators bound the inactive conformations with significant preference using both docking programs, and 6 out of 9 cases (67%), the positive modulators bound the active conformations. Considering results by the individual programs only, even higher correlations were observed: 12/14 (86%) and 8/9 (89%) for ArgusLab and 10/14 (71%) and 7/9 (78%) for AutoDock. These findings strongly support the hypothesis that mGluR allosteric modulation occurs via stabilization of different conformations analogous to those identified in rhodopsin where they are induced by photochemical isomerization of the retinal ligand--despite the extensive differences in sequences between mGluRs and rhodopsin.     

Covalent Bond between Ligand and Receptor Required for Efficient Activation in Rhodopsin

Rhodopsin is an extensively studied member of the G protein-coupled receptors (GPCRs). Although rhodopsin shares many features with the other GPCRs, it exhibits unique features as a photoreceptor molecule. A hallmark in the molecular structure of rhodopsin is the covalently bound chromophore that regulates the activity of the receptor acting as an agonist or inverse agonist. Here we show the pivotal role of the covalent bond between the retinal chromophore and the lysine residue at position 296 in the activation pathway of bovine rhodopsin, by use of a rhodopsin mutant K296G reconstituted with retinylidene Schiff bases. Our results show that photoreceptive functions of rhodopsin, such as regiospecific photoisomerization of the ligand, and its quantum yield were not affected by the absence of the covalent bond, whereas the activation mechanism triggered by photoisomerization of the retinal was severely affected. Furthermore, our results show that an active state similar to the Meta-II intermediate of wild-type rhodopsin did not form in the bleaching process of this mutant, although it exhibited relatively weak G protein activity after light irradiation because of an increased basal activity of the receptor. We propose that the covalent bond is required for transmitting structural changes from the photoisomerized agonist to the receptor and that the covalent bond forcibly keeps the low affinity agonist in the receptor, resulting in a more efficient G protein activation.     

Agonists and partial agonists of rhodopsin: retinals with ring modifications

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