Literature DB >> 29899455

Structure of the µ-opioid receptor-Gi protein complex.

Antoine Koehl1, Hongli Hu1,2, Shoji Maeda2, Yan Zhang1,2, Qianhui Qu1,2, Joseph M Paggi1,2,3,4, Naomi R Latorraca1,2,3,4,5, Daniel Hilger2, Roger Dawson6, Hugues Matile6, Gebhard F X Schertler7,8, Sebastien Granier9, William I Weis1,2, Ron O Dror1,2,3,4,5, Aashish Manglik10,11, Georgios Skiniotis12,13, Brian K Kobilka14.   

Abstract

The μ-opioid receptor (μOR) is a G-protein-coupled receptor (GPCR) and the target of most clinically and recreationally used opioids. The induced positive effects of analgesia and euphoria are mediated by μOR signalling through the adenylyl cyclase-inhibiting heterotrimeric G protein Gi. Here we present the 3.5 Å resolution cryo-electron microscopy structure of the μOR bound to the agonist peptide DAMGO and nucleotide-free Gi. DAMGO occupies the morphinan ligand pocket, with its N terminus interacting with conserved receptor residues and its C terminus engaging regions important for opioid-ligand selectivity. Comparison of the μOR-Gi complex to previously determined structures of other GPCRs bound to the stimulatory G protein Gs reveals differences in the position of transmembrane receptor helix 6 and in the interactions between the G protein α-subunit and the receptor core. Together, these results shed light on the structural features that contribute to the Gi protein-coupling specificity of the µOR.

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Year:  2018        PMID: 29899455      PMCID: PMC6317904          DOI: 10.1038/s41586-018-0219-7

Source DB:  PubMed          Journal:  Nature        ISSN: 0028-0836            Impact factor:   49.962


The μOR is the primary target of morphine and many clinically used opioid analgesics[1]. Opioid binding to the μOR leads to clinically desired analgesic and antitussive actions but also important negative side effects including addiction and potentially lethal respiratory suppression. Opioids have become the most prescribed class of medication in the United States[2], leading to a national epidemic of addiction and an unprecedented level of drug overdose deaths. Like other GPCRs, the μOR achieves many of its physiological actions by stimulating signaling via a heterotrimeric G protein. While other GPCRs have been shown to signal through more than one G protein subtype, the μOR signals almost exclusively through the adenylyl-cyclase inhibitory family of G proteins (Gi/o)[3]. The analgesic activity of opioids is driven by G protein activation[4], but activated μOR can also interact with β-arrestins, whose recruitment has been associated with the respiratory depression induced by many opioids[5,6]. Recently developed molecules that favor Gi signaling over arrestin recruitment display analgesic efficacy with reduced side effects, suggesting that different signaling pathways can be selectively targeted to yield unique physiological outcomes[7,8]. Though a framework for GPCR interactions with the stimulatory G protein Gs has recently been enabled by X-ray crystallography[9] and cryo-electron microscopy (cryo-EM)[10,11], the structural basis for GPCR signaling through other G protein subtypes remains undefined. To better understand the mechanism of selective activation of Gi by the μOR, we sought to determine the structure of the μOR-Gi complex.

3.5-Å cryo-EM map of a μOR-Gi complex

DAMGO (H-Tyr-D-Ala-Gly-N-MePhe-Gly-OH) is a μOR-selective synthetic analog of the natural peptide agonist enkephalin. DAMGO-bound μOR was incubated with Gi1 heterotrimer and the complex was treated with the nucleotide hydrolase apyrase to remove GDP. The resulting nucleotide-free complex was further stabilized by a single-chain variable fragment (scFv16) that binds to heterotrimeric Gi (Extended Data Figure 1) and prevents GTPγS mediated dissociation of nucleotide-free complexes. We applied single-particle cryo-EM to initially obtain a three-dimensional map of the μOR-DAMGO-Gi-scFv16 complex at an indicated nominal resolution of 3.6 Å (Extended Data Fig. 2–3, Extended Data Table 1). Notably, scFv16 binds a composite interface comprised of the αN helix of Gαi and the β propeller of Gβ, a site that is more than 20 Å distal to the μOR-Gαi interface and does not perturb the interface between Gα and Gβ subunits (Extended Data Figure 1). Subtraction of the scFv16 signal from raw particle images led to an improved map with an indicated global resolution of 3.5 Å. This map displayed enhanced features particularly in the receptor transmembrane core (Extended Data Figures 2, 3, 4), enabling the high resolution visualization of the μOR-Gi interface and ligand binding. Accordingly, we employed this improved 3.5-Å map to examine interactions between μOR and DAMGO, and between μOR and Gi (Fig. 1a, b).
Extended Data Figure 1

scFv binding characteristics

scFv 16 does not perturb the interfaces between Gα and Gβ at a) its binding epitope or b) the Switch II region located ~40A away. Our structure is colored by chain, while the structure of GDP-bound Gi1 heterotrimer (PDB 1GP2) is colored grey. c) In the nucleotide-free state, there is a ~7˚ rotation of G βγ relative to the Gαs Switch II domain when compared to the GDP-bound form. This rotated conformation is similar to that observed in nucleotide-free Gs coupled to the β2AR (PDB ID 3SN6) as shown in panel d).

Extended Data Figure 2

Cryo-EM data processing

a, Representative cryo-EM micrograph of the μOR-Gi complex. Scale bar, 20nm.

b, Representative two-dimensional averages showing distinct secondary structure features from different views of the complex.

c, Flow chart of cryo-EM data processing. The unmasked map in the middle of the chart has been colored by subunit. The inset shows the fit of the crystal structure of the α-helical domain in the corresponding density of the unmasked reconstruction. Three-dimensional density maps colored according to local resolution.

d, “Gold standard” Fourier shell correlation (FSC) curves from Phenix indicates overall nominal resolutions of 3.5 Å and 3.6 Å using the FSC=0.143 criterion for the scFv-subtracted map (green curve) and scFv-retained maps (purple curve), respectively.

Extended Data Figure 3

Cryo-EM map vs. refined structure

a) EM density map (scFv subtracted) and model are shown for all seven transmembrane α-helices of the μOR, DAMGO, and Gα helices α5 and αN.

b,c) Cross-validation of model to EM density map. The model was refined against one half map after displacement of atoms by 0.2A, and FSC curves were calculated between this model and the final cryo-EM map (full dataset, black), of the outcome of model refinement with a half map versus the same map (red), and of the outcome of model refinement with a half map versus the other half map (green). The results of the scFv-retained model vs. map and of scFv subtracted model vs. map are shown in b) and c), respectively.

Extended Data Table 1

Cryo-EM data collection, refinement and validation statistics

μOR-Gi Complex (EMDB-xxxx) (PDB xxxx)μOR-Gi-scFvl6 Complex (EMDB-yyyy) (PDB yyyy)
Data collection and processing
Magnification48,07648,076
Voltage (kV)300300
Electron exposure (e–/Å2)4040
Defocus range (μm)−0.8 ~ −2.6−0.8 ~ −2.6
Pixel size (Å)1.041.04
Symmetry imposedC1C1
Initial particle images (no.)893,426893,426
Final particle images (no.)359,406359,406
Map resolution (Å)3.5 Å3.6 Å
 FSC threshold(0.143)(0.143)
Map resolution range (Å)3.3-4.53.3-4.5
Refinement
Initial model used (PDB code)5C1M1GP25C1M1GP2
Model resolution (Å)3.53.6
Model resolution range (Å)3.3-4.53.3-4.5
Map sharpening B factor (Å2)Pre −90, post −60Pre −90, post −60
Model composition
 Non-hydrogen atoms69868731
 Protein residues886 residues (6949 atoms)1119 residues (8694 atoms)
 Ligands1 (37 atoms)1 (37 atoms)
B factors (Å2)
 Protein33.2360.55
 Ligand31.2779.99
R.m.s. deviations
 Bond lengths (Å)0.0070.007
 Bond angles (°)1.3111.015
Validation
 MolProbity score1.891.89
 Clashscore7.028.16
 Poor rotamers (%)0.720.92
Ramachandran plot
 Favored (%)91.5492.93
 Allowed (%)8.356.98
 Disallowed (%)0.11%0.09%
Extended Data Figure 4

Selected cryo-EM densities of μOR-Gi Complex

Cryo-EM density (displayed as mesh) surrounding residues involved in a) DAMGO binding, b) μOR-Gαi interaction around ICL2, c) ICL3, and d) cytoplasmic ends of the μOR transmembrane helices. These figures accompany the models shown in figures 1e, 4b, 5a, and 5b respectively.

Figure 1

Cryo-EM structure of the μOR-Gi complex

a, Orthogonal views of the cryo-EM density map of the μOR-Gi heterotrimer complex colored by subunit (μOR in green, DAMGO in orange, G⍺s Ras-like domain in gold, Gβ in cyan, Gγ in purple). b, Model of the μOR-Gi complex in the same views and color scheme as shown in a. c, Residues that line the μOR orthosteric binding pocket are shown as sticks for the μOR-Gi complex (green) and the μOR-Nb39 complex (PDB 5C1M; blue). The binding pocket residues of DAMGO and BU-72 occupied μOR show nearly identical conformations, despite differences in ligand structure. d, Comparison of BU-72 (yellow carbons) in the orthosteric pocket of the μOR-Nb39 complex (blue) with DAMGO (orange carbons) in the orthosteric pocket of the μOR-Gi complex (green). e, view of DAMGO in the orthosteric binding pocket with critical residues shown. f, A frame from every 100 ns of a 1 μs MD simulation (yellow for t = 0 fading to red for t = 1 μs) shows that the first 4 residues of DAMGO (bottom) are stable, whereas the C-terminal Gly-ol (top) is dynamic but frequently returns to the modeled pose.

Activation of μOR by a peptide agonist

We previously determined the active-state crystal structure of μOR bound to the morphinan agonist BU72 and an active-state stabilizing nanobody (Nb39) at a resolution of 2.2 Å12. Like other small molecule morphinans, BU72 is rigidified by a complex ring system, in contrast to flexible opioid peptides like DAMGO that have multiple rotatable bonds. The cryo-EM map includes well-defined features for most amino acids forming the orthosteric binding pocket (Extended Data Fig. 4a). Despite differences in agonist structure, the conformation of the active-state binding pocket and the orientation of the amino acids that interact with the agonist are highly similar for the μOR bound to BU72 or DAMGO (Fig. 1c), suggesting that the μOR recognizes structurally distinct agonists in a stereotypic manner. Although DAMGO is a flexible ligand, we observe density for the entire peptide bound to the receptor (Fig. 1a, Extended Data Fig. 3, 4). The DAMGO N-terminus occupies a similar position in the binding pocket as BU72. In contrast, the C-terminus of DAMGO extends ~8 Å further towards the extracellular loops compared to BU72 (Fig. 1d, e). To identify stable atomic-level interactions between DAMGO and the binding pocket, we performed molecular (MD) dynamics simulations. In over 1μs of simulation, DAMGO remained close to its initially modeled pose, with the amino-terminal portion largely remaining confined to the experimentally determined EM density (Fig. 1f, Extended Data Fig 5). The DAMGO N-terminus maintained a persistent salt bridge with D1473.32, a feature previously observed in structures of morphinans bound to opioid receptors (Fig. 1e; superscripts indicate Ballesteros-Weinstein numbering for GPCRs[13]). The same amine group also often formed a hydrogen bond with Y3267.43. More generally, the amino-terminal Tyr of DAMGO overlaps the phenolic group of other small molecule opioids characterized previously by X-ray crystallography[14-17].
Extended Data Figure 5

Stability of DAMGO in MD Simulations

a. Over the course of MD simulations, the positions of the first 4 residues of DAMGO do not significantly change, while the 5th residue (Gly-ol) shows significant variability in position. Frames from the first and last 100 ns are shown with an intermediate to highlight both the relative stability of the first 4 amino acids, as well as the flexibility of the fifth. Arrows show the extent of motion in the N- and C-terminal residues over the course of simulation. Cryo-EM density for DAMGO is shown as mesh.

b. Root mean standard deviations (RMSDs) from the modeled pose of DAMGO to the pose during MD simulations. The RMSD calculations include heavy atoms on the peptide backbone. Data from three independent simulations are plotted. The RMSDs for residues 1 to 4 (black) and the C-terminal Gly-ol (blue) are plotted separately to highlight their stability and mobility, respectfully.

MD simulations also revealed a water-mediated hydrogen bonding network that closely overlaps with the water network observed in the high-resolution crystal structure of μOR[12] (Extended Data Fig. 6). In particular, the simulations revealed a stable, water-mediated interaction formed between the DAMGO phenol and H2976.52. Though the crystal structure of the μOR bound to BU-72 shows two water molecules bridging the DAMGO phenol and H2976.52, simulations of μOR bound to DAMGO and other phenolic ligands[8,12] suggest that one of these waters rapidly dissociates and that a single water is required for stable ligand binding. This interaction is a hallmark of opioid recognition that has been observed for morphinans in complex with the μOR[12,14] as well as other small molecule and peptide-mimetic agonists for the homologous δ and κ opioid receptors (κOR)[15,16,18].
Extended Data Figure 6

Water occupancy in orthosteric binding site

Left panel, water occupancy in MD simulations of DAMGO-bound μOR overlaid with a representative conformation from MD simulations. ‘Occupancy relative to bulk solvent’ is the ratio of the rate at which water is observed in a given volume to the rate at which water is expected to be observed in an equivalent volume in the bulk solvent. For example, blue regions (occupancy ratio = 2) are occupied by water twice as often as an equivalent region in the bulk solvent. Right panel, crystallographic waters in the BU72-bound μOR binding pocket (PDB ID: 5C1M). Waters are shown as black spheres, BU72 is shown as yellow sticks, and hydrogen bonds are shown as dashed lines.

DAMGO is more than 500-fold selective for the μOR over the δOR and κOR[19]. As elucidated in prior structures, ligand interactions with the extracellular loops encode ligand subtype specificity among closely related opioid receptors[15]. Indeed, DAMGO selectivity for μOR over δOR has been shown to result from residues in ECL1 while selectivity over κOR results from differences in ECL3[20]. The map density for the carboxy-terminal residues of DAMGO is slightly weaker than for the amino-terminus, consistent with increased mobility of this region in simulations (Fig. 1f, Extended Data Fig 5). In our model, the DAMGO N-Me-Phe side chain occupies a conserved hydrophobic pocket near ECL1 and the Gly-OH group folds back over the ligand (Fig. 1e). This model is consistent with the high affinity μOR binding of cyclized enkephalins that bridge the +2 and +5 positions of the peptide[21].

Structure of Gi-Stabilized Active μOR

The overall structure of Gi-bound μOR is similar to the active conformation of the BU72-bound μOR stabilized by Nb39 (root mean square deviation of 1 Å)[12] with a predominant outward displacement of TM6 from the heptahelical bundle relative to the inactive state (Fig. 2a, b). A number of highly conserved residues in the GPCR family have been shown to be important for receptor activation, including the D3.49R3.50Y3.51, the N7.49P7.50xxY7.53, and conserved core triad (I3.40, P5.50, and F6.44) motifs. The conformation of each of these regions in the μOR-Gi complex is virtually identical to the active state observed in complex with Nb39 (Fig. 2c). The structural similarity of μOR between Nb39 and Gi-coupled states indicate that these changes underlie ligand-mediated activation and are not specific to a particular intracellular binder. Indeed, Nb39 and Gi promote a similar increase in agonist affinity[12], which supports a common mechanism of allosteric communication between the intracellular G protein coupling domain and the ligand binding pocket[12].
Figure 2

Structural changes in the μOR stabilized by nucleotide-free Gi

a, Comparison of inactive μOR (brown) and the Gi stabilized active state of μOR (green). b, Comparison of Nb39 and Gi stabilized active states of the μOR (blue and green, respectively). The structures are nearly identical except for a slight shift of TM6 towards TM7 in the Gi -bound state. c, Residues important for activation of the μOR show nearly identical conformations despite the difference in ligands. d, Comparison of Gs-stabilized β2AR (orange) and Gi-stabilized μOR (green). While most transmembrane helices align well between the two receptors, TM6 is kinked further outward by 9Å in the β2AR. Distance calculated between Cα of residue 6.29 (Ballesteros-Weinstein numbering) in TM6.

Two differences between Nb39 and Gi stabilized active-states of μOR are particularly notable. First, compared with the nanobody-stabilized active-state μOR, TM6 in the μOR-Gi complex is further displaced by 3 Å towards TM7 (Fig. 2b). Second, the conformation of intracellular loop 3 (ICL3) is different in the two structures (Fig. 2a). It is likely that the specific ICL3 conformation of μOR stabilized by Nb39 reflects interactions that are unique to the nanobody rather than a general feature of receptor activation prior to G protein coupling. A similar difference in ICL3 conformation was previously observed for the β2-adrenergic receptor (β2AR) between nanobody (Nb80)[22] and Gs-coupled states. The comparison of the G protein bound states of both receptors shows that the β2AR TM6 is displaced outward by another 9 Å compared to the μOR (Fig. 2d).

Structural Changes in Gi

The quality of the cryo-EM map enabled accurate modeling of Gi in its nucleotide-free state, providing insight into the structural changes that underlie nucleotide release. The changes we observe are similar to those observed in nucleotide-free Gs in complex with other GPCRs. The most striking difference between the GDP bound[23] and nucleotide free heterotrimer in complex with μOR involves the separation of the α-helical domain (AHD) from the Ras-like domain in the alpha subunit of Gi (Gαi) (Fig. 3a). Due to its relative flexibility, we excluded the AHD density from the high-resolution map refinement. The dynamic character of the AHD has been observed previously by spectroscopic and structural studies in complexes between receptors and both Gs[9-11] and Gi[24,25]. Displacement of the AHD disrupts several contacts with GDP and is necessary, but not sufficient for nucleotide release, a process that involves breaking additional contacts with the Ras domain[24].
Figure 3

Changes in Gi upon coupling to the μOR

a, b, Comparison of GDP-bound Gαi (PDB 1GP2, grey) and nucleotide-free Gαi from the μOR-Gi complex (gold). GDP is shown as blue spheres in panel a and sticks in panel b. The primary differences between these two structures are the opening and outward movement of the alpha helical domain (AHD), and an upward shift of the α5 helix by 6Å to engage the receptor core. The α-carbons of the TCAT motif are represented as spheres in panel b. The TCAT motif coordinates the guanosine base of GDP. The upward shift of the α5 helix and repositioning of the TCAT motif leads to nucleotide release. c, d, e, The interface between the α1 helix and the N-terminal end of the α5 helix and TCAT motif for GDP-bound Gαi (c), nucleotide free Gαi (d), and nucleotide free Gs from the β2AR -Gs complex (e). The upward movement of the α5 helix disrupts the interaction between the α1 and α5 helices leading to changes in the P-loop that coordinates the phosphates of GDP.

Gi coupling to the μOR also involves a 6-Å translation as well as a 60° rotation of the Gαi α5 helix into the receptor core (Fig. 3b). This movement has been shown to be essential for nucleotide release in Gi[24]. In particular, the motion of α5 leads to a change in the position of the β6-α5 loop containing the conserved TCAT motif that forms direct interactions with the guanine base of GDP. This displacement disrupts key contacts between the G protein and nucleotide. Furthermore, the observed translation and rotation of the α5 helix requires the displacement of the fully conserved F336 away from the hydrophobic pocket formed by residues in the β2/β3 strands and the α1 helix[26] (Fig. 3b). Movement of the α5 helix is also propagated to the phosphate binding P-loop connecting the β1 strand and the α1 helix by disruption of a hydrophobic network between the α1 and α5 helices (Fig. 3b–d). Correspondingly, upon transition of Gi to the nucleotide-free state, we observe a 4-Å shift of α1 towards the α5 helix in Gi whereby the hydrophobic contacts are replaced by polar interactions with the β6-α5 loop as it is released from its guanine binding position (Fig. 3c, d). These changes contrast those observed in structures of Gs-coupled complexes, in which α1 not only becomes more unstructured, but also tends to lose interactions with the α5 helix (Fig. 3e). Our structure is consistent with previous studies suggesting that engagement of a GPCR with the α5 helix and αN- β1 loop leads to concerted changes in the α1 helix and P loop that destabilize contacts with the guanine nucleotide leading to its release[27].

Structural insights into Gi coupling specificity of the μOR

Although the μOR couples exclusively to Gi/o[3], many GPCRs can couple to multiple G protein subtypes; a well-studied example is the β2AR, which couples to both Gs and Gi/o. Prior sequence-level analyses have failed to identify a linear GPCR epitope that determines G protein coupling specificity, suggesting that it is likely determined by a more complex three-dimensional network of interactions. Globally, the structure of the μOR-Gi complex is similar to the β2AR-Gs, likely reflecting a similarity in the conformation of nucleotide-free states of Family A GPCR-G protein complexes. The primary interaction sites in both complexes occur between ICL2, ICL3 and TMs 3,5, and 6 on the receptor and the αN, αN- β1 loop, and α5 helix on the Gα subunit of the G protein (Fig. 4). The most striking difference between the β2AR-Gs and μOR-Gi complex is in the relative position of the α5 helix of both G proteins, as well as the corresponding shift in the position of TM6 of the receptor. The α5 helix of Gαi is rotated ~21° relative to the α5 helix of Gαs, leading to a 5 Å displacement of the extreme C-terminus of the Gαi helix α5 toward TM7 of the μOR (Fig. 4a). This difference in α5 positioning is associated with a smaller outward displacement of the μOR TM6. The C-terminal residues of α5 that interact with TMs 5 and 6 of the receptor are bulkier in Gs than in Gi, with Y and E compared to C and G at positions −4 and −3 from the C-terminus, respectively. Accordingly, substitution of these two amino acids of Gs into Gi would lead to steric clashes with TM3 and the TM7-Helix 8 loop (Extended Data Fig. 7). In the Gs-coupled Family B calcitonin[11] and GLP-1[10] receptors, G protein coupling is associated with a large kink of TM6 at the conserved PxxG motif, which produces an even larger outward displacement of TM6 than what observed in the β2AR-Gs complex.
Figure 4

Comparison of the receptor-G protein binding interfaces of the μOR-Gi and β2AR-Gs complexes

a, Comparison of the conformation of the α5 helix of Gα and receptor TM6 in β2AR-Gs and μOR-Gi complexes after alignment on the receptor. b, Interactions between ICL2 of the μOR (green) and Gαi (gold). Asp 350 of Gαi is depicted with narrow lines to indicate uncertainty in its conformation due to poor cryo-EM density for its side chain. c, Interactions between ICL2 of the β2AR (orange) and Gαs (blue). d, Surface view of the hydrophobic pockets in Gαi (top panel) and Gαs (bottom panel) that interact with a non-polar amino acid in ICL2 of the μOR and β2AR, respectively.

Extended Data Figure 7

Comparison of the C-termini of Gαs and Gαi

The C-terminus of Gαs is bulkier than that of Gαi due to substitution of small amino acids C (−4 position) and G (−3 position) in Gαi to Y and E respectively in Gαs. This leads to steric clashes with TMs 3 and 7 of the μOR.

Top - ribbon view of μOR (green) with WT Gαi (gold, left) and a Gαis model (right) created by substituting C and G for Y and E based on the β2AR-Gs crystal structure. Substituted positions are colored in light purple. The −4 to −2 positions have their side chains shown as spheres, and the rest as a ribbon.

Bottom - space filling view of the μOR showing the steric clashes that result from these substitutions.

Surprisingly, the structure of μOR-Gi shows substantial similarity to an active-state structure of the visual pigment rhodopsin (Meta II) in complex with a modified peptide derived from the 11 C-terminal residues of the α subunit of the visual G protein transducin (GαtCT2) (Extended Data Fig. 8)[28]. Despite the lack of the remainder of the heterotrimeric G protein in the MetaII- GαtCT2 structure, the conformation of TM6 of MetaII is highly similar to that of the μOR, while the location of the GαtCT2 peptide is almost identical to the C-terminus of Gi in complex with μOR. This finding is consistent with observations that substitution of the last five amino acids of the Gα α5 helix is sufficient to change G protein coupling specificity[29].
Extended Data Figure 8

Comparison of Gai C terminal peptide binding modes

Side (top half), and cytoplasmic (bottom half) views of a) the μOR (green) with the last 11 residues of Gαi (gold) alone, b) compared to the β2AR(orange) with the last 11 residues of Gαs (light purple) (PDB ID 3SN6), or c) compared to MetaII Rhodopsin (pink) in complex with an 11 residue Gtransducin (Gt) C-terminal peptide (dark purple) (PDB ID 3PQR). The mOR-Gi complex aligns best with the MetaII-Gt complex both in terms of TM6 displacement as well as position of the α5 peptide.

In Extended Data Table 2, we list amino acids in the μOR that interact with the cytoplasmic surface of Gi. The μOR ICL2 primarily forms interactions with the αN and α5 helices of Gαi, including a key ionic interaction between the μOR D17734.55 [G Protein Coupled Receptor Data Base (GPCRDB) numbering[30]] in ICL2 and R32 in the αN- β1 loop of Gαi (Fig. 4b). Although D34.55 in ICL2 is conserved in all opioid receptors with available sequences (GPCRDB[31]), it is variable in most other Gi coupled receptors. Another notable interaction involves R17934.57 in μOR ICL2, which simultaneously coordinates the highly conserved D1643.49 in the DRY motif and potentially forms an additional interaction with D350 in the Gαi α5 helix (−5 position) (Fig. 4b). This arginine is essential for μOR induced Gi signaling, as the polymorphic variant R179C abolishes signaling in vitro[32] and leads to insensitivity to morphine in patients homozygous for the mutation[33]. The potential role of this interaction network in G protein coupling is supported by the preponderance of basic residues (arginine and lysine) at this position in most Gi coupled receptors, whereas Gs-coupled receptors employ alternative residues (Extended Data Table 2).
Extended Data Table 2

Sequence alignment of residues that form the interaction interface between μOR and Gi. Receptors from different branches of the GPCR family with different coupling specificity were selected for analysis. Sequences and alignment were performed using GPCRDB (gpcrdb.org)

CouplingBranch
mOR ResidueT103V169P172V173D177R179T180M255K271R277I278
2.393.5434.5034.5134.5534.574.385.616.266.326.33
[Human] 5-HT1A receptorGiαAIPINRTIAKT
[Human] 5-HT1B receptorGiαAIAVARTIMKA
[Human] M2 receptorGiαNVPLVRTIPKV
[Human] M4 receptorGiαNVPLARTIMKV
[Human] alpha2A-adrenoceptorGiαQIAILRTIRRF
[Human] FPR1GiγTVPVNRTIRP
[Human] FPR2/ALXGiγTVPVNRTIRP
[Human] GAL1 receptorGiγTISRSRVVKT
[Human] GAL3 receptorGiγTVPLARTTRRA
[Human] δ receptorGiγTVPVDRTMKRI
[Human] κ receptorGiγTVPVDRTMKRI
[Human] μ receptorGiγTVPVDRTMKRI
[Human] NOP receptorGiγTIPIDRTMKRI
[Human] SST1 receptorGiγTVPIRRRIRKI
[Human] SST2 receptorGiγTVPIKRRIRKV
[Human] SST3 receptorGiγTVPTRRTIRRV
[Human] SST4 receptorGiγTVPLTRRIRKI
[Human] SST5 receptorGiγTVPLRRRIKV
[Human] CCR1GiγTIAVRRTIKA
[Human] CCR4GiγTIAVRRTIKA
[Human] CXCR4GiγTIATRRKIKA
[Human] A1 receptorGiαTVPLMVTVYKI
[Human] beta1-adrenoceptorGsαTIPFSLTVVKA
[Human] beta2-adrenoceptorGsαTIPFSLTVFKA
[Human] MC1 receptorGsαMIALSVTGKG
[Human] MC2 receptorGsαMIALSVTKKG
[Human] MC4 receptorGsαMIALNMTRKG
[Human] A2A receptorGsαTIPLGVTITHA
[Human] H2 receptorGsαTVPLVVTIAKA
[Human] TA1 receptorGsαTVPLAMNISKA
[Human] RXFP1GsδYIPFRGMQIL
[Human] RXFP2GsδHIPFRGMCAV
[Human] V2 receptorGsβIIPMRGSIVKT
[Human] 5-HT2A receptorGqαTIPIRNSTSKA
[Human] 5-HT2B receptorGqαTIPIQNSTTRA
[Human] M1 receptorGqαNVPLARTISKA
[Human] M3 receptorGqαNIPLARTISKA
[Human] M5 receptorGqαNIPLARTIVKA
[Human] alpha1A-adrenoceptorGqαTVPLTVTVKKA
[Human] GAL2 receptorGqγTIPLERTTAKV
[Human] OX1 receptorGqβTIPLTIQKT
[Human] OX2 receptorGqβTIPLTIQKT
[Human] NK1 receptorGqβTISVQKV
A further group of contacts occurs between P17234.50 and V17334.51 of μOR and a hydrophobic patch on Gαi comprised of residues F336, I343, I344, and T340 on the α5 helix and L194 on the β2- β3 loop (Fig. 4b, d). In the GDP bound state, these α5 helix residues are buried by the adjacent β2 and β3 loops. Coupling to a receptor involves an upward shift of the α5 helix and exposes these residues to form a shallow hydrophobic pocket that interacts with μOR V17334.51 in ICL2 (Fig. 4b, d). In the case of Gs, a deeper hydrophobic pocket in this region engages the bulky aromatic F13934.51 in ICL2 of the β2AR (Fig. 4c, d). In the μOR, ICL3 stabilizes the interface between receptor and G protein through two sets of interactions: one set involves multiple contacts with a hydrophobic patch on the α5 helix of Gαi, while another engages the β6 strand of Gαi through a network of charged residues (Fig. 5a, b). The hydrophobic interface formed by ICL3 is similar in both the μOR and β2AR; in the β2AR, TM5 is helically extended to form a larger hydrophobic interaction around nonpolar residues in the α5 helix of Gαs (Fig. 5c, d). While the shorter ICL3 of the μOR does not form a similar helical extension, it nevertheless fulfills the same role. Residues V2625.68, M264 and L265 fold back to form a hydrophobic patch that interacts with hydrophobic residues on the α5 helix of Gαi (Figure 5a).
Figure 5

Comparison of the receptor-G protein binding interfaces of the μOR-Gi and β2AR-Gs complexes

Top panels show interactions between ICL3 of μOR and Gαi (a) and between the cytosolic ends of TMs 3,5,6, of the μOR and the α5 helix of Gi (b). Asp 350 of Gαi is depicted with narrow lines to indicate uncertainty in its position due to poor cryo-EM density for its side chain. Bottom panels show these same interfaces between β2AR and Gs (c,d).

The second set of polar contacts involves μOR R263 and a backbone carbonyl to I319 on the β6 strand of Gαi (Fig. 5a). Mutations of R263 reduce, but do not abolish, Gi signaling[34], which is consistent with the potential importance of stabilizing the Gαi β6 strand in the observed conformation. A similar interaction is absent in the β2AR-Gs complex (Fig. 5c). This additional recognition interface may be necessary for efficient μOR-Gi coupling due to the higher affinity for GDP to Gi relative to Gs. Compared to Gs-coupled receptors, additional interactions with the β6 strand in Gi-coupled receptors may be required to disrupt interactions between the Ras domain and GDP for efficient nucleotide exchange. The cytosolic ends of μOR TMs 3,5 and 6 further stabilize the nucleotide-free conformation of the α5 helix by interacting with highly conserved residues in the distal C-terminus of Gαi (Figure 5b). In particular, C351 (−4 position) of Gαi is in close proximity to the cytosolic end of μOR TM3. This cysteine residue has previously been identified as the site of pertussis toxin-mediated inhibition of Gi/o family proteins by enzymatic ADP-ribosylation[35]. The close apposition of C351 to the μOR cytoplasmic surface highlights how the addition of a bulky modification at this position can completely inhibit receptor coupling and nucleotide exchange[35]. In addition to this interaction, μOR residues M2555.61, I2786.33, M2816.36, and V2826.37 form a hydrophobic pocket that engages the absolutely conserved Gαi residue L353 (−2 position) in the α5 helix. Methionines M2555.61 and M2816.36 have previously been observed in NMR experiments to respond to activation by DAMGO[36], suggesting that this region undergoes conformational changes prior to G protein coupling. Further stabilization, however, is likely provided by a hydrogen bond between R2776.32 and the backbone carbonyl of L353 (Fig. 5b). Notably, interactions between the C-terminus of the α5 helix and the receptor core are entirely different in the in the β2AR-Gs complex (Fig. 5c). Our findings provide structural insights into the inability of the μOR to couple to Gs, but do not explain the mechanism of G protein coupling specificity across all GPCRs. It is possible that coupling specificity is determined at an intermediate step in the formation of a GPCR-G protein complex, such as the initial interactions between the GDP-bound G protein and the agonist-bound receptor. Recent single molecule fluorescence studies provide evidence for a transient intermediate complex between GDP-bound Gs and the β2AR that is associated with a smaller outward movement of TM6[37]. Previous studies suggest that amino acids C-terminal to helix 8 confer coupling specificity for Gq in the M3 muscarinic receptor (M3R)[38]. Given that there are no interactions between the C-terminus of the β2AR or μOR with their respective G proteins in the nucleotide-free complexes, we postulate that engagement of Gq and the M3R C-terminus may occur at an earlier stage in complex formation. Thus, the nucleotide-free GPCR-G protein complex may be preceded by one or more GDP-bound intermediates characterized by dynamic low affinity interactions with the receptor. Such initial encounter complexes may have larger energetic differences for interactions with various G protein subtypes than the nucleotide-free state, and would thereby contribute more critically to coupling specificity. The transient nature of such interactions, however, currently poses challenges for structure determination by both crystallography and cryo-EM.

METHODS

Online Methods

No statistical methods were used to predetermine sample size. The experiments were not randomized and the investigators were not blinded to allocation during experiments and outcome assessment.

Purification of μ-opioid receptor

These studies utilized a previously described mouse μOR construct with cleavable amino and carboxy terminal domains[12]. Briefly, the receptor was expressed in Spodoptera frugiperda Sf9 insect cells using the baculovirus method (Expression Systems), extracted from insect cell membranes with n-dodecyl-β-D-maltoside (DDM, Anatrace), and purified by nickel-chelating sepharose chromatography. The Ni-NTA eluate was loaded onto M1 anti-FLAG immunoaffinity resin and washed with progressively lower concentrations of the antagonist naloxone. The μOR was then eluted in a buffer consisting of 20 mM Hepes pH 7.5, 100 mM NaCl, 0.1% DDM, 0.01% cholesterol hemisuccinate (CHS) supplemented with 50 nM naloxone, FLAG peptide and 5 mM EDTA. The monomeric fraction was purified by size exclusion chromatography on a Superdex 200 10/300 gel filtration column (GE) in 20 mM Hepes pH 7.5, 100 mM NaCl, 0.1% DDM, 0.01% CHS, and 1 μM DAMGO. A further 2-fold molar excess of DAMGO was added to the preparation and the resulting agonist-bound μOR preparation was concentrated to ~100 μM.

Expression and purification of heterotrimeric Gi

Heterotrimeric Gi was expressed and purified as previously described[24]. Briefly, Trichuplusia ni Hi5 insect cells were coinfected with two viruses, one encoding the wild-type human Gαi subunit and another encoding the wild-type human β1γ2 subunits with an octahistidine tag inserted at the amino terminus of the β1 subunit. Cultures were harvested 48 hours post infection. Cells were lysed in hypotonic buffer and lipid-modified heterotrimeric Gi was extracted in a buffer containing 1% sodium cholate. The soluble fraction was purified using Ni-NTA chromatography, and the detergent was exchanged from cholate to DDM on column. After elution, the protein was dialyzed against a buffer containing 20 mM Hepes pH 7.5, 100 mM NaCl, 0.015% DDM, 100 μM TCEP, 10 μM GDP, and concentrated to ~20 mg/mL for further complexing with the μOR.

Generation of scFv16

6–8 week old female Balb/c mice were immunized with a purified rhodopsin-Gi complex[39]. Hybridoma cells were prepared using splenocytes of immunized mice using standard methods in combination with PAI myeloma cells. Clones that showed a positive reaction to purified rhodopsin(N2C/D282C/M257Y)/Gi1 complex in an ELISA assay and by immunoprecipitation were further characterized as monoclonal antibodies or Fab fragments. Fab-16 was selected from the initial pool of clones because it prevented dissociation of the rhodopsin (N2C/D282C/M257Y)/Gi1 complex by GTPγS, and therefore acted as a stabilizing chaperone in the same manner as Nb35 for Gs. The full sequence of constructs used is listed in Supplemental Figure 1. All animal studies were performed at Roche Innovation Center Basel according to ethical guidelines. All cell lines were obtained from manufacturer and tested for contamination. A carboxy-terminal hexahistidine-tagged single chain construct of Fab16 (scFv16) was cloned into a modified pVL1392 vector containing a GP67 secretion signal immediately prior to the amino terminus of the scFv, expressed in secreted form from Trichuplusia ni Hi5 insect cells using the baculoviral method, and purified by Ni-NTA chromatography. Supernatant from baculoviral infected cells was pH balanced by addition of Tris pH 8.0. Chelating agents were quenched by addition of 1 mM nickel chloride and 5 mM calcium chloride and incubation with stirring for 1 hr at 25 °C. Resulting precipitates were removed by centrifugation and the supernatant was loaded onto Ni-NTA resin. The column was washed with 20 mM Hepes pH 7.5, 500 mM NaCl, and 10 mM imidazole followed by a low salt wash comprised of the same buffer substituted with 100 mM NaCl. Following elution with the same buffer supplemented with 250 mM imidazole, the carboxy-terminal hexahistidine tag was cleaved by incubation with human rhinovirus 3C protease, and the protein was dialyzed into a buffer consisting of 20mM Hepes pH 7.5 and 100 mM NaCl. Cleaved scFv16 was further purified by reloading over Ni-NTA resin. The flow-through was collected and purified over gel filtration chromatography using a Superdex 200 16/60 column. Monomeric fractions were pooled, concentrated, and flash frozen in liquid nitrogen until further use.

Formation and purification of the μOR-Gi-scFv16 complex

Purified DAMGO-bound μOR was mixed with a 1.2 molar excess of Gi heterotrimer. The coupling reaction was allowed to proceed at 24 °C for 1 hour and was followed by addition of apyrase to catalyze hydrolysis of unbound GDP, which destabilizes the nucleotide-free complex[40]. After one more hour at 25 °C, a 4-fold volume of 20 mM Hepes pH 7.5, 100 mM NaCl, 1% lauryl maltose neopentyl glycol (L-MNG), 0.1% CHS was added to the complexing reaction to initiate detergent exchange. After one hour incubation at 25 °C to allow micelle exchange, 1 mM MnCl2 and lambda phosphatase (New England Biolabs) were added to dephosphorylate the preparation. This reaction was further incubated at 4 °C for 2 hours. To remove excess G protein and residual DDM, the complexing mixture was purified by M1 anti-FLAG affinity chromatography. Bound complex was first washed in a buffer containing 1% L-MNG, followed by washes in gradually decreasing L-MNG concentrations. The complex was then eluted in 20mM Hepes pH 7.5, 100mM NaCl, 0.01% MNG/0.001% CHS, 300 nM DAMGO, 5 mM EDTA, and FLAG peptide. The eluted complex was supplemented with 100 μM TCEP to provide a reducing environment. The tobacco etch virus (TEV) protease and human rhinovirus 3C protease were added to cleave the flexible μOR amino- and carboxy- termini. Finally, a 1.2 molar excess of scFv16 was added to the preparation. Once cleavage of the termini was confirmed by SDS-PAGE, the μOR-Gi-scFv16 complex was purified by size exclusion chromatography on a Superdex 200 10/300 column in 20mM Hepes pH 7.5, 100mM NaCl, 300 nM DAMGO, 0.00075% MNG and 000025% GDN. Peak fractions were concentrated to ~7 mg/mL for electron microscopy studies.

Cryo-electron microscopy of μOR-Gi-scFv16 complex

3.0 μL of purified μOR-Gi-scFv16 complex was applied to glow-discharged 200 mesh grids (Quantifoil R1.2/1.3) and subsequently vitrified using a Vitrobot Mark IV (Thermo Fischer Scientific). Cryo-EM imaging was performed on a Titan Krios operated at 300 kV at a nominal magnification of 130,000x using a Gatan K2 Summit direct electron camera in counted mode, corresponding to a pixel size of 1.04 Å. A total of 2642 image stacks were obtained with a defocus range of −0.8 to −2.6 μm. Each stack movie was recorded for a total of 8 seconds with 0.1s per frame. The dose rate was 5 e/Å2/s, resulting in an accumulated dose of 40 electrons per Å2. Dose fractionated image stacks were subjected to beam-induced motion correction using MotionCor2[41]. A sum of all frames, filtered according to exposure dose, in each image stack was used for further processing. CTF parameters for each micrograph were determined by Gctf v1.06[42]. Particle selection, two-dimensional and three-dimensional classification, and 3D reconstruction were performed using RELION2.1[43], apart from the last round of local refinement and reconstruction that was performed with Frealign[44]. Semi-automated selected 893,426 particle projections were subjected to reference-free two-dimensional classification and averaging using a binned data set with a pixel size of 2.08 Å. 379,373 particles belonging to well-defined averages were subjected to further processing. An ab initio map generated by VIPER[45] was used as initial reference model for maximum-likelihood-based three-dimensional classification, which, however did not produce classes with notable differences. Thus, all 379,373 particle projections were subjected to 3D refinement, producing a map at 4.3 Å resolution. The dataset was further reduced by removing particle projections from micrographs with resolution lower than 4.5 Å, resulting in a data set of 359,406 particles that were subjected to refinement and reconstruction after subtracting densities for the mobile Gα α-helical domain and the detergent micelle[11]. Particle projection assignments from RELION were imported into Frealign[46] for a final round of local refinement and reconstruction. To prevent overfitting, the resolution limit for every alignment iteration never exceeded the 0.9 value of the Frealign calculated FSC. The map was further improved map after additionally subtracting densities corresponding to the ScFv from the raw particle projections[11]. The indicated resolution, using Phenix “gold standard” FSC[47], of the final reconstruction is 3.5 Å and 3.6 Å at FSC 0.143 for the ScFv subtracted map and the ScFv including map, respectively. Local resolution was determined using the Bsoft package[48] with unfiltered half-maps as input.

Model Building and Refinement

The building of a full atomic model for the μOR-Gi complex was aided by the quality and resolution of our map, as well as the existence of high-resolution crystal structures of each of the components that make up the complex. A composite model was formed by rigid body fitting of the active-state μOR (PDB ID: 5C1M)[12] with nanobody removed, as well as the Ras domain and βγ subunits of GDP-bound Gi (PDB ID: 1GP2)[23]. The α5 helix of Gαi was removed and manually fit to the density, and the final 8 residues missing from the extreme C-terminus of the 1GP2 structure were manually built in coot[49]. This starting model was then subjected to iterative rounds of automated refinement in Rosetta[50] and Phenix real space refine[47], and manual building in Coot[49]. In the regions of the model for which side chain density was too weak to unambiguously assign a conformation, we stubbed residues to their C βposition, while preserving sequence information (Supplemental Figure 2,3). The final model was visually inspected for general fit to the map, and geometry was further evaluated using Molprobity[51] as part of the Phenix suite of software. Initial restraints for DAMGO were generated using the PRODRG server[52]. To further refine the pose of DAMGO, we chose a pose from molecular dynamics simulation consistent with our map and then performed a refinement using Phenix. This involved manually editing the residue and atom names from a CHARMM parameter file to match the 3-letter codes and atom names from the rcsb. In particular, DAL for D-alanine, MEA for N-methyl phenylalanine, and ETA for Gly-ol C terminus. Additional, custom, restraints were generated to keep planarity of the final peptide bond between MEA and ETA as a supplement to the natural library of phenix amino acid restraints. Model overfitting was evaluated through its refinement against one cryo-EM half map after randomly displacing all atoms by 0.2 Å. FSC curves were calculated between the resulting model and the half map used for refinement (green curve, Extended Data Fig. 2b, c), as well as between the resulting model and the other half map for cross- validation (blue curve, Extended Data Fig. 2b, c), and also against the full map (red curve, Extended Data Fig. 2b, c). The final refinement statistics for both models are provided in Extended Data Table 1.

System setup for molecular dynamics simulations

Molecular dynamics simulations were initiated from an earlier refinement of the structure reported in this study after removing the G protein and ScFv fragment. Prior to beginning simulations, Schrödinger Glide[53] was used to relax DAMGO to an energetically favorable conformation. The initial DAMGO pose is depicted in Extended Data Figure 3. We performed five independent simulations, for each of which initial atom velocities were assigned randomly and independently. Prime (Schrödinger, Inc.) was used to model missing side chains, and neutral acetyl and methylamide groups were added to cap protein termini. Titratable residues remained in their dominant protonation state at pH 7, as determined using PropKa, except for D2.50 and D3.49 which were protonated. Our simulations incorporated the waters from the 5C1M crystal structure. The prepared protein structures were aligned to the Orientation of Proteins in Membranes (OPM) structure for PDB entry 5C1M[54]. The aligned structures were then inserted into a pre-equilibrated palmitoyl-oleoyl-phosphatidylcholine (POPC) bilayer using Dabble, a simulation preparation software[55]. Sodium and chloride ions were added to neutralize each system at a concentration of approximately 150 mM. Bilayer dimensions were chosen to maintain at least a 30 Å buffer between protein images in the x-y plane and a 20 Å buffer between protein images in the z direction. Final system dimensions were approximately 80 × 75 × 90 Å3. Simulation times for each replicate were approximately 1 μs.

Molecular dynamics simulation protocols

We used the CHARMM36m force field for proteins, lipids, and ions and the TIP3P model for waters[56-60]. Parameters for the non-canonical residues in DAMGO were determined by analogy to N-methyl glycine for assigning N-methyl parameters to N-methyl phenylalanine (residue 4) and by analogy to serine to assign parameters to the Gly-ol capping group (residue 5). CMAP terms for D-alanine were inverted from those for L-Alanine to account for the inverted chirality of the residue. We performed the simulations using the Compute Unified Device Architecture (CUDA) version of Particle-Mesh Ewald Molecular Dynamics (PMEMD) in AMBER on one or two graphical processing units (GPUs)[61]. Simulations were performed using the AMBER16[62] software. Three rounds of minimization were performed, each consisting of 500 iterations of steepest descent minimization, followed by 500 iterations of conjugate gradient descent minimization, with harmonic restraints of 10.0, 5.0, and 1.0∙kcal∙mol−1∙Å−2 placed on the protein and lipids. Systems were heated from 0K to 100K in the NVT ensemble over 12.5 ps and then from 100K to 310K in the NPT ensemble over 125 ps, using 10.0∙kcal∙mol−1∙Å−2 harmonic restraints applied to lipid and protein heavy atoms. Systems were then equilibrated at 310 K in the NPT ensemble at 1 bar, with harmonic restraints on all protein heavy atoms tapered off by 1.0 kcal∙mol−1∙Å−2 starting at 5.0∙kcal∙mol−1∙Å−2 in a stepwise fashion every 2 ns for 10 ns and then by 0.1 kcal∙mol−1∙Å−2 in a stepwise fashion every 2 ns for 20 ns. Production simulations were performed in the NPT ensemble at 310K and 1 bar, using a Langevin thermostat for temperature coupling and a Monte Carlo barostat for pressure coupling. These simulations used a 4 fs time step with hydrogen mass repartitioning[63]. Bond lengths to hydrogen atoms were constrained using SHAKE. Simulations used periodic boundary conditions. Non-bonded interactions were cut off at 9.0 Å, and long-range electrostatic interactions were computed using Particle Mesh Ewald (PME) with an Ewald coefficient of approximately 0.31 Å and an interpolation order of 4. The FFT grid size was chosen such that the width of a grid cell was approximately 1 Å. During production simulations, all residues within 5 Å of the G protein interface were restrained to the initial structure using 5.0 kcal∙mol−1∙Å−2 harmonic restraints applied to non-hydrogen atoms. Using such restraints reduces the overall system size, enabling more simulation, while ensuring that the receptor maintains an active conformation throughout the simulation.

Analysis protocols for MD simulation

Trajectory snapshots were saved every 200 ps during production simulations. The AmberTools17 CPPTRAJ package was used to reimage and center trajectories[64]. Simulations were visualized and analyzed using Visual Molecular Dynamics (VMD)[65]. In two simulations, DAMGO was trapped in an unstable binding pose, wherein the water-mediated interaction between the DAMGO Tyr residue and His297 failed to form during equilibration, and instead a direct hydrogen bond between these residues was formed. Our analysis is based on the other three simulations, in which DAMGO’s pose was consistent with the EM density. Water occupancy maps were generated using AmberTools17 GIST[66,67]. Frames from every 1 ns of simulation, excluding the first 400 ns, aligned to the initial structure, were used as input. The grid size was set to 0.25 Å. The resulting map was smoothed using a Gaussian filter with a standard deviation of 2 grid cells.

scFv binding characteristics

scFv 16 does not perturb the interfaces between Gα and Gβ at a) its binding epitope or b) the Switch II region located ~40A away. Our structure is colored by chain, while the structure of GDP-bound Gi1 heterotrimer (PDB 1GP2) is colored grey. c) In the nucleotide-free state, there is a ~7˚ rotation of G βγ relative to the Gαs Switch II domain when compared to the GDP-bound form. This rotated conformation is similar to that observed in nucleotide-free Gs coupled to the β2AR (PDB ID 3SN6) as shown in panel d).

Cryo-EM data processing

a, Representative cryo-EM micrograph of the μOR-Gi complex. Scale bar, 20nm. b, Representative two-dimensional averages showing distinct secondary structure features from different views of the complex. c, Flow chart of cryo-EM data processing. The unmasked map in the middle of the chart has been colored by subunit. The inset shows the fit of the crystal structure of the α-helical domain in the corresponding density of the unmasked reconstruction. Three-dimensional density maps colored according to local resolution. d, “Gold standard” Fourier shell correlation (FSC) curves from Phenix indicates overall nominal resolutions of 3.5 Å and 3.6 Å using the FSC=0.143 criterion for the scFv-subtracted map (green curve) and scFv-retained maps (purple curve), respectively.

Cryo-EM map vs. refined structure

a) EM density map (scFv subtracted) and model are shown for all seven transmembrane α-helices of the μOR, DAMGO, and Gα helices α5 and αN. b,c) Cross-validation of model to EM density map. The model was refined against one half map after displacement of atoms by 0.2A, and FSC curves were calculated between this model and the final cryo-EM map (full dataset, black), of the outcome of model refinement with a half map versus the same map (red), and of the outcome of model refinement with a half map versus the other half map (green). The results of the scFv-retained model vs. map and of scFv subtracted model vs. map are shown in b) and c), respectively.

Selected cryo-EM densities of μOR-Gi Complex

Cryo-EM density (displayed as mesh) surrounding residues involved in a) DAMGO binding, b) μOR-Gαi interaction around ICL2, c) ICL3, and d) cytoplasmic ends of the μOR transmembrane helices. These figures accompany the models shown in figures 1e, 4b, 5a, and 5b respectively.

Stability of DAMGO in MD Simulations

a. Over the course of MD simulations, the positions of the first 4 residues of DAMGO do not significantly change, while the 5th residue (Gly-ol) shows significant variability in position. Frames from the first and last 100 ns are shown with an intermediate to highlight both the relative stability of the first 4 amino acids, as well as the flexibility of the fifth. Arrows show the extent of motion in the N- and C-terminal residues over the course of simulation. Cryo-EM density for DAMGO is shown as mesh. b. Root mean standard deviations (RMSDs) from the modeled pose of DAMGO to the pose during MD simulations. The RMSD calculations include heavy atoms on the peptide backbone. Data from three independent simulations are plotted. The RMSDs for residues 1 to 4 (black) and the C-terminal Gly-ol (blue) are plotted separately to highlight their stability and mobility, respectfully.

Water occupancy in orthosteric binding site

Left panel, water occupancy in MD simulations of DAMGO-bound μOR overlaid with a representative conformation from MD simulations. ‘Occupancy relative to bulk solvent’ is the ratio of the rate at which water is observed in a given volume to the rate at which water is expected to be observed in an equivalent volume in the bulk solvent. For example, blue regions (occupancy ratio = 2) are occupied by water twice as often as an equivalent region in the bulk solvent. Right panel, crystallographic waters in the BU72-bound μOR binding pocket (PDB ID: 5C1M). Waters are shown as black spheres, BU72 is shown as yellow sticks, and hydrogen bonds are shown as dashed lines.

Comparison of the C-termini of Gαs and Gαi

The C-terminus of Gαs is bulkier than that of Gαi due to substitution of small amino acids C (−4 position) and G (−3 position) in Gαi to Y and E respectively in Gαs. This leads to steric clashes with TMs 3 and 7 of the μOR. Top - ribbon view of μOR (green) with WT Gαi (gold, left) and a Gαis model (right) created by substituting C and G for Y and E based on the β2AR-Gs crystal structure. Substituted positions are colored in light purple. The −4 to −2 positions have their side chains shown as spheres, and the rest as a ribbon. Bottom - space filling view of the μOR showing the steric clashes that result from these substitutions.

Comparison of Gai C terminal peptide binding modes

Side (top half), and cytoplasmic (bottom half) views of a) the μOR (green) with the last 11 residues of Gαi (gold) alone, b) compared to the β2AR(orange) with the last 11 residues of Gαs (light purple) (PDB ID 3SN6), or c) compared to MetaII Rhodopsin (pink) in complex with an 11 residue Gtransducin (Gt) C-terminal peptide (dark purple) (PDB ID 3PQR). The mOR-Gi complex aligns best with the MetaII-Gt complex both in terms of TM6 displacement as well as position of the α5 peptide. Cryo-EM data collection, refinement and validation statistics Sequence alignment of residues that form the interaction interface between μOR and Gi. Receptors from different branches of the GPCR family with different coupling specificity were selected for analysis. Sequences and alignment were performed using GPCRDB (gpcrdb.org)
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1.  PRODRG: a tool for high-throughput crystallography of protein-ligand complexes.

Authors:  Alexander W Schüttelkopf; Daan M F van Aalten
Journal:  Acta Crystallogr D Biol Crystallogr       Date:  2004-07-21

2.  Grid inhomogeneous solvation theory: hydration structure and thermodynamics of the miniature receptor cucurbit[7]uril.

Authors:  Crystal N Nguyen; Tom Kurtzman Young; Michael K Gilson
Journal:  J Chem Phys       Date:  2012-07-28       Impact factor: 3.488

3.  MolProbity: More and better reference data for improved all-atom structure validation.

Authors:  Christopher J Williams; Jeffrey J Headd; Nigel W Moriarty; Michael G Prisant; Lizbeth L Videau; Lindsay N Deis; Vishal Verma; Daniel A Keedy; Bradley J Hintze; Vincent B Chen; Swati Jain; Steven M Lewis; W Bryan Arendall; Jack Snoeyink; Paul D Adams; Simon C Lovell; Jane S Richardson; David C Richardson
Journal:  Protein Sci       Date:  2017-11-27       Impact factor: 6.725

4.  The ribosome at improved resolution: new techniques for merging and orientation refinement in 3D cryo-electron microscopy of biological particles.

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Journal:  Ultramicroscopy       Date:  1994-03       Impact factor: 2.689

5.  The Phenix software for automated determination of macromolecular structures.

Authors:  Paul D Adams; Pavel V Afonine; Gábor Bunkóczi; Vincent B Chen; Nathaniel Echols; Jeffrey J Headd; Li-Wei Hung; Swati Jain; Gary J Kapral; Ralf W Grosse Kunstleve; Airlie J McCoy; Nigel W Moriarty; Robert D Oeffner; Randy J Read; David C Richardson; Jane S Richardson; Thomas C Terwilliger; Peter H Zwart
Journal:  Methods       Date:  2011-07-29       Impact factor: 3.608

6.  Inclusion of many-body effects in the additive CHARMM protein CMAP potential results in enhanced cooperativity of α-helix and β-hairpin formation.

Authors:  Robert B Best; Jeetain Mittal; Michael Feig; Alexander D MacKerell
Journal:  Biophys J       Date:  2012-09-05       Impact factor: 4.033

7.  A G protein-biased ligand at the μ-opioid receptor is potently analgesic with reduced gastrointestinal and respiratory dysfunction compared with morphine.

Authors:  Scott M DeWire; Dennis S Yamashita; David H Rominger; Guodong Liu; Conrad L Cowan; Thomas M Graczyk; Xiao-Tao Chen; Philip M Pitis; Dimitar Gotchev; Catherine Yuan; Michael Koblish; Michael W Lark; Jonathan D Violin
Journal:  J Pharmacol Exp Ther       Date:  2013-01-08       Impact factor: 4.030

8.  Structure of the human κ-opioid receptor in complex with JDTic.

Authors:  Huixian Wu; Daniel Wacker; Mauro Mileni; Vsevolod Katritch; Gye Won Han; Eyal Vardy; Wei Liu; Aaron A Thompson; Xi-Ping Huang; F Ivy Carroll; S Wayne Mascarella; Richard B Westkaemper; Philip D Mosier; Bryan L Roth; Vadim Cherezov; Raymond C Stevens
Journal:  Nature       Date:  2012-03-21       Impact factor: 49.962

9.  Single-molecule analysis of ligand efficacy in β2AR-G-protein activation.

Authors:  G Glenn Gregorio; Matthieu Masureel; Daniel Hilger; Daniel S Terry; Manuel Juette; Hong Zhao; Zhou Zhou; Jose Manuel Perez-Aguilar; Maria Hauge; Signe Mathiasen; Jonathan A Javitch; Harel Weinstein; Brian K Kobilka; Scott C Blanchard
Journal:  Nature       Date:  2017-06-07       Impact factor: 49.962

10.  RELION: implementation of a Bayesian approach to cryo-EM structure determination.

Authors:  Sjors H W Scheres
Journal:  J Struct Biol       Date:  2012-09-19       Impact factor: 2.867

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2.  Molecular mechanism of biased signaling in a prototypical G protein-coupled receptor.

Authors:  Carl-Mikael Suomivuori; Naomi R Latorraca; Laura M Wingler; Stephan Eismann; Matthew C King; Alissa L W Kleinhenz; Meredith A Skiba; Dean P Staus; Andrew C Kruse; Robert J Lefkowitz; Ron O Dror
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3.  Illuminating G-Protein-Coupling Selectivity of GPCRs.

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Review 4.  Understanding Peptide Binding in Class A G Protein-Coupled Receptors.

Authors:  Irina G Tikhonova; Veronique Gigoux; Daniel Fourmy
Journal:  Mol Pharmacol       Date:  2019-07-10       Impact factor: 4.436

5.  Structural basis for GPCR-independent activation of heterotrimeric Gi proteins.

Authors:  Nicholas A Kalogriopoulos; Steven D Rees; Tony Ngo; Noah J Kopcho; Andrey V Ilatovskiy; Nina Sun; Elizabeth A Komives; Geoffrey Chang; Pradipta Ghosh; Irina Kufareva
Journal:  Proc Natl Acad Sci U S A       Date:  2019-07-30       Impact factor: 11.205

6.  Conformational plasticity of the intracellular cavity of GPCR-G-protein complexes leads to G-protein promiscuity and selectivity.

Authors:  Manbir Sandhu; Anja M Touma; Matthew Dysthe; Fredrik Sadler; Sivaraj Sivaramakrishnan; Nagarajan Vaidehi
Journal:  Proc Natl Acad Sci U S A       Date:  2019-05-28       Impact factor: 11.205

Review 7.  Function-related conformational dynamics of G protein-coupled receptors revealed by NMR.

Authors:  Takumi Ueda; Yutaka Kofuku; Junya Okude; Shunsuke Imai; Yutaro Shiraishi; Ichio Shimada
Journal:  Biophys Rev       Date:  2019-05-17

8.  Optogenetic Modulation of Ion Channels by Photoreceptive Proteins.

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9.  Molecular dynamics of fentanyl bound to μ-opioid receptor.

Authors:  Piotr F J Lipiński; Małgorzata Jarończyk; Jan Cz Dobrowolski; Joanna Sadlej
Journal:  J Mol Model       Date:  2019-05-03       Impact factor: 1.810

Review 10.  The structural basis of the arrestin binding to GPCRs.

Authors:  Vsevolod V Gurevich; Eugenia V Gurevich
Journal:  Mol Cell Endocrinol       Date:  2019-01-28       Impact factor: 4.102

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