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. 1. Department of Structural Biology, Stanford University School of Medicine, Stanford, CA, USA. 2. Department of Molecular and Cellular Physiology, Stanford University School of Medicine, Stanford, CA, USA. 3. Department of Computer Science, Stanford University, Stanford, CA, USA. 4. Institute for Computational and Mathematical Engineering, Stanford University, Stanford, CA, USA. 5. Biophysics Program, Stanford University, Stanford, CA, USA. 6. Roche Pharma Research and Early Development, Therapeutic Modalities, Roche Innovation Center Basel, F.Hoffmann-La Roche, Basel, Switzerland. 7. Laboratory of Biomolecular Research, Paul Scherrer Institute, Villigen, Switzerland. 8. Department of Biology, ETH Zürich, Zürich, Switzerland. 9. Institut de Génomique Fonctionnelle, INSERM, Montpellier, France. 10. Department of Pharmaceutical Chemistry, University of California San Francisco, San Francisco, CA, USA. Aashish.Manglik@ucsf.edu. 11. Department of Anesthesia and Perioperative Care, University of California San Francisco, San Francisco, CA, USA. Aashish.Manglik@ucsf.edu. 12. Department of Structural Biology, Stanford University School of Medicine, Stanford, CA, USA. yiorgo@stanford.edu. 13. Department of Molecular and Cellular Physiology, Stanford University School of Medicine, Stanford, CA, USA. yiorgo@stanford.edu. 14. Department of Molecular and Cellular Physiology, Stanford University School of Medicine, Stanford, CA, USA. kobilka@stanford.edu.
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.
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.
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
Magnification
48,076
48,076
Voltage (kV)
300
300
Electron exposure
(e–/Å2)
40
40
Defocus range (μm)
−0.8 ~ −2.6
−0.8 ~ −2.6
Pixel size (Å)
1.04
1.04
Symmetry imposed
C1
C1
Initial particle images (no.)
893,426
893,426
Final particle images (no.)
359,406
359,406
Map resolution (Å)
3.5 Å
3.6 Å
FSC threshold
(0.143)
(0.143)
Map resolution range (Å)
3.3-4.5
3.3-4.5
Refinement
Initial model used (PDB code)
5C1M1GP2
5C1M1GP2
Model resolution (Å)
3.5
3.6
Model resolution range (Å)
3.3-4.5
3.3-4.5
Map sharpening B factor
(Å2)
Pre −90, post −60
Pre −90, post −60
Model composition
Non-hydrogen atoms
6986
8731
Protein residues
886 residues (6949 atoms)
1119 residues (8694 atoms)
Ligands
1 (37 atoms)
1 (37 atoms)
B factors
(Å2)
Protein
33.23
60.55
Ligand
31.27
79.99
R.m.s. deviations
Bond lengths (Å)
0.007
0.007
Bond angles (°)
1.311
1.015
Validation
MolProbity score
1.89
1.89
Clashscore
7.02
8.16
Poor rotamers (%)
0.72
0.92
Ramachandran plot
Favored (%)
91.54
92.93
Allowed (%)
8.35
6.98
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 BU72orDAMGO (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 DAMGON-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
μORTM6. 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)
Coupling
Branch
mOR Residue
T103
V169
P172
V173
D177
R179
T180
M255
K271
R277
I278
2.39
3.54
34.50
34.51
34.55
34.57
4.38
5.61
6.26
6.32
6.33
[Human] 5-HT1A receptor
Gi
α
A
I
P
I
N
R
T
I
A
K
T
[Human] 5-HT1B receptor
Gi
α
A
I
A
V
A
R
T
I
M
K
A
[Human] M2 receptor
Gi
α
N
V
P
L
V
R
T
I
P
K
V
[Human] M4 receptor
Gi
α
N
V
P
L
A
R
T
I
M
K
V
[Human] alpha2A-adrenoceptor
Gi
α
Q
I
A
I
L
R
T
I
R
R
F
[Human] FPR1
Gi
γ
T
V
P
V
N
R
T
I
–
R
P
[Human] FPR2/ALX
Gi
γ
T
V
P
V
N
R
T
I
–
R
P
[Human] GAL1 receptor
Gi
γ
T
I
S
R
S
R
V
V
–
K
T
[Human] GAL3 receptor
Gi
γ
T
V
P
L
A
R
T
T
R
R
A
[Human] δ receptor
Gi
γ
T
V
P
V
D
R
T
M
K
R
I
[Human] κ receptor
Gi
γ
T
V
P
V
D
R
T
M
K
R
I
[Human] μ receptor
Gi
γ
T
V
P
V
D
R
T
M
K
R
I
[Human] NOP receptor
Gi
γ
T
I
P
I
D
R
T
M
K
R
I
[Human] SST1 receptor
Gi
γ
T
V
P
I
R
R
R
I
R
K
I
[Human] SST2 receptor
Gi
γ
T
V
P
I
K
R
R
I
R
K
V
[Human] SST3 receptor
Gi
γ
T
V
P
T
R
R
T
I
R
R
V
[Human] SST4 receptor
Gi
γ
T
V
P
L
T
R
R
I
R
K
I
[Human] SST5 receptor
Gi
γ
T
V
P
L
R
R
R
I
–
K
V
[Human] CCR1
Gi
γ
T
I
A
V
R
R
T
I
–
K
A
[Human] CCR4
Gi
γ
T
I
A
V
R
R
T
I
–
K
A
[Human] CXCR4
Gi
γ
T
I
A
T
R
R
K
I
–
K
A
[Human] A1 receptor
Gi
α
T
V
P
L
M
V
T
V
Y
K
I
[Human] beta1-adrenoceptor
Gs
α
T
I
P
F
S
L
T
V
V
K
A
[Human] beta2-adrenoceptor
Gs
α
T
I
P
F
S
L
T
V
F
K
A
[Human] MC1 receptor
Gs
α
M
I
A
L
S
V
T
G
–
K
G
[Human] MC2 receptor
Gs
α
M
I
A
L
S
V
T
K
–
K
G
[Human] MC4 receptor
Gs
α
M
I
A
L
N
M
T
R
–
K
G
[Human] A2A receptor
Gs
α
T
I
P
L
G
V
T
I
T
H
A
[Human] H2 receptor
Gs
α
T
V
P
L
V
V
T
I
A
K
A
[Human] TA1 receptor
Gs
α
T
V
P
L
A
M
N
I
S
K
A
[Human] RXFP1
Gs
δ
Y
I
P
F
R
–
G
M
Q
I
L
[Human] RXFP2
Gs
δ
H
I
P
F
R
–
G
M
C
A
V
[Human] V2 receptor
Gs
β
I
I
P
M
R
G
S
I
V
K
T
[Human] 5-HT2A receptor
Gq
α
T
I
P
I
R
N
S
T
S
K
A
[Human] 5-HT2B receptor
Gq
α
T
I
P
I
Q
N
S
T
T
R
A
[Human] M1 receptor
Gq
α
N
V
P
L
A
R
T
I
S
K
A
[Human] M3 receptor
Gq
α
N
I
P
L
A
R
T
I
S
K
A
[Human] M5 receptor
Gq
α
N
I
P
L
A
R
T
I
V
K
A
[Human] alpha1A-adrenoceptor
Gq
α
T
V
P
L
T
V
T
V
K
K
A
[Human] GAL2 receptor
Gq
γ
T
I
P
L
E
R
T
T
A
K
V
[Human] OX1 receptor
Gq
β
T
I
P
L
–
–
T
I
Q
K
T
[Human] OX2 receptor
Gq
β
T
I
P
L
–
–
T
I
Q
K
T
[Human] NK1 receptor
Gq
β
T
I
–
–
–
–
S
V
Q
K
V
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
μORTM3. 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 frugiperdaSf9 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 orFab
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-methylphenylalanine, 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 DAMGOTyr 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 statisticsSequence 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)
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
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
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
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
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
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 Journal: Science Date: 2020-02-21 Impact factor: 47.728
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
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