Heterodimeric integrin adhesion receptors regulate cell migration, survival and differentiation in metazoa by communicating signals bi‐directionally across the plasma membrane. Protein engineering and mutagenesis studies have suggested that the dissociation of a complex formed by the single‐pass transmembrane (TM) segments of the α and β subunits is central to these signalling events. Here, we report the structure of the integrin αIIbβ3 TM complex, structure‐based site‐directed mutagenesis and lipid embedding estimates to reveal the structural event that underlies the transition from associated to dissociated states, that is, TM signalling. The complex is stabilized by glycine‐packing mediated TM helix crossing within the extracellular membrane leaflet, and by unique hydrophobic and electrostatic bridges in the intracellular leaflet that mediate an unusual, asymmetric association of the 24‐ and 29‐residue αIIb and β3 TM helices. The structurally unique, highly conserved integrin αIIbβ3 TM complex rationalizes bi‐directional signalling and represents the first structure of a heterodimeric TM receptor complex.
The family of integrin cell adhesion receptors regulates cell migration, survival and differentiation in metazoa by responding to intracellular and extracellular signals in inside‐out and outside‐in signalling pathways, respectively (Hynes, 2002; Askari et al, 2009; Harburger and Calderwood, 2009). Integrins are Type I heterodimeric receptors that consist of large extracellular domains (>700 residues), single‐pass transmembrane (TM) segments and generally short cytosolic tails (<70 residues). Integrin αIIbβ3, the primary adhesion receptor of blood platelets, mediates platelet aggregation by binding to the multivalent blood protein fibrinogen (Hynes, 2002; Bennett, 2005). It is essential to both the arrest of bleeding at sites of vascular injury and pathological thrombosis culminating in heart attack and stroke. The sequences of the TM segments of the 18 α and 8 β human subunits are well conserved (Figure 1), and the TM region of integrin αIIbβ3 closely resembles many of the 18 α and 8 β human subunits, in particular the distinct, hydrophobic sequences C‐terminal to the first charged residues on the intracellular side, αIIb(K989) and β3(K716). Integrin bi‐directional TM signalling involves the dissociation of a complex formed by the α–β TM segments (Hughes et al, 1996; Kim et al, 2003; Li et al, 2005; Partridge et al, 2005; Zhu et al, 2007), which is accompanied by large rearrangements of its extracellular domains (Xiao et al, 2004; Adair et al, 2005; Rocco et al, 2008; Ye et al, 2008; Zhu et al, 2008). Recently, we have determined the structures and lipid embedding of the monomeric integrin αIIb and β3 TM segments in phospholipid bicelles (Lau et al, 2008a, 2008b), laying the foundation for understanding the structural transition between dissociated and associated TM states, and thus integrin αIIbβ3 TM signalling. Although the monomeric β3 TM segment forms a 29‐residue α‐helix that is tilted in the membrane and immerses β3(K716), the αIIb segment adopts a straight, 24‐residue TM helix that terminates at αIIb(K989). C‐terminal to the αIIb helix an unusual Gly‐Phe‐Phe backbone reversal is observed that immerses the two fully conserved Phe residues (Figure 1) back into the intracellular membrane leaflet (Lau et al, 2008a).
Many structural models of the signalling events in the membrane have been proposed and the structural information on the monomeric, dissociated αIIb and β3 TM states increases the possible structural transitions between the associated and dissociated state even further. In general, changes in the TM segment membrane crossing angles accompanying lateral separation of the TM segments pictured in helical conformation are predicted (Luo et al, 2004; Gottschalk, 2005; Li et al, 2005; Partridge et al, 2005; Wegener et al, 2007). In such an event, the Gly‐Phe‐Phe motif may convert to helical conformation, as suggested by reported cytosolic αIIbβ3 tail complex structures (Vinogradova et al, 2002; Weljie et al, 2002) and induce an αIIb TM helix elongation and tilt that may favour a modelled Glycophorin A‐like αIIbβ3 association (Gottschalk, 2005). Alternatively, the five‐residue hydrophobic stretch C‐terminal to the first charged residues on the intracellular side of the β3 subunit, K716, may repartition into the cytosol, leading to a straight β3 TM helix and a more parallel αIIbβ3 TM association. Moreover, membrane embedding of the TM helices may also change at the extracellular face in a piston‐like manner and thereby transmit a force to the integrin ectodomain. Finally, a direct association between the monomeric αIIb–β3 TM structures may occur, which would be the first example of an asymmetric, heterodimeric TM association. Here, we report the structure of the noncovalently associated αIIbβ3 TM complex, structure‐based site‐directed mutagenesis and lipid embedding estimates to differentiate the plethora of integrin TM signalling possibilities. Aside from providing insight into integrin biology, the integrin αIIbβ3 TM complex structure also advances the understanding of dimeric cell receptor TM complexes of which only homodimeric structures have been reported (MacKenzie et al, 1997; Call et al, 2006; Bocharov et al, 2007, 2008).
Results and discussion
Integrin αIIb–β3 heterodimerization and structure determination
The structure of the noncovalently associated αIIbβ3 TM complex was determined in the phospholipid bilayer environment of small bicelles (Lee et al, 2008); this is essential for obtaining accurate integrin TM conformations (Lau et al, 2008b) and was achieved by solution NMR spectroscopy using peptides of several different 2H/13C/15N labelling patterns. Random mutagenesis of the β3 TM segment and the entire cytosolic tail shows that the used peptides, encompassing αIIb(A958‐P998) and β3(P685‐F727), contain all TM and cytosolic αIIbβ3 heterodimerization elements (Partridge et al, 2005). Under the chosen experimental conditions, the mixing of αIIb and β3 peptides resulted in the presence of the monomeric NMR resonances obtained earlier (Lau et al, 2008a, 2008b) and a new set of resonances, corresponding to the associated αIIbβ3 state (Figure 2A and B). All backbone resonance positions and, hence, the structures and chemical environment of the co‐existing monomers and heterodimer were independent of αIIb‐to‐β3 peptide ratio and lipid‐to‐peptide ratio (Figure 2C). In analogy to the monomeric αIIb and β3 TM structures (Lau et al, 2008a, 2008b), no significant variation in backbone chemical shifts and, hence, αIIbβ3 complex structure was found between the herein used lipids of 16/18 and 14/14 carbon atom tails, and phosphocholine and serine headgroups (data not shown), which represent the major platelet lipids (GarciaGuerra et al, 1996). Incomplete, but dominant, heterodimerization in bicelles (Figure 2C) agrees with a relatively weak αIIbβ3 TM association detected in Escherichia coli membranes (Li et al, 2004; Schneider & Engelman, 2004), although the truncated TM segments used in these earlier studies may have unduly favoured homodimerization over heterodimerization. The αIIbβ3 association was sensitive to the integrity of the proposed αIIb(R995)–β3(D723) salt bridge (Hughes et al, 1996), as the introduction of the αIIb(R995A) substitution essentially led to the loss of heterodimeric resonances (Figure 2C; Supplementary Figure 2A and B). However, αIIb(R995A) did not abrogate the heterodimeric association completely. The signal intensities of the monomeric resonances still experienced significant reductions in the presence of αIIb(R995A) peptide (Supplementary Figure 2C). This indicates the presence of additional heterodimerization elements and, on the timescale of the NMR measurements, reflects a transition from the slow to the fast exchange limit. In conclusion, the αIIb and β3 TM segments associate quantitatively and specifically in phospholipid bicelles with contributions from αIIb(R995)–β3(D723) electrostatic interactions and additional heterodimerization elements.
The observation of separate, nonaveraged signals for monomeric and heterodimeric protein backbone resonances (slow exchange limit; Figure 2) allows for the direct backbone structure determination of these co‐existing species and a simultaneous comparison of their lipid embedding. It shows as well that complex dissociation is relatively slow in bicelles, taking place on the millisecond timescale, but association is also slow as heterodimerization is incomplete. Slow exchange behaviour was also observed at the level of side chain resonances, but, more often, monomeric and heterodimeric signals were averaged, resulting in only one resonance (fast exchange limit; Figure 3). The behaviour of a resonance to exhibit fast or slow exchange depends, in addition to the underlying exchange kinetics, on the chemical shift (frequency) difference between monomeric and heterodimeric states (Cavanagh et al, 1996). As the monomeric αIIb and β3 TM structures are already known (Lau et al, 2008a, 2008b), they can serve as a convenient reference for assessing any possible change in backbone conformation on heterodimerization. Secondary 13Cα chemical shifts exhibit a high correlation with backbone conformation and low dependence on the chemical environment (Spera and Bax, 1991; Xu and Case, 2001), which makes them the most sensitive NMR parameter for assessing backbone structural changes. The secondary 13Cα chemical shifts between monomeric and heterodimeric states are essentially superimposable (Figure 4). Minor 13Cα chemical shift differences at the intracellular membrane face are well within expected margins from the stabilization of secondary structures, particularly the two C‐terminal β3 helix turns, by heterodimerization involving the newly formed αIIb(R995)–β3(D723) salt bridge. Thus, a transition of the distinct αIIb(G991‐F992‐F993) backbone reversal to helical conformations can be excluded. H–N chemical shifts, on the other hand, exhibit a low correlation with backbone conformation and high dependence on the chemical environment (Wagner et al, 1983; Wang and Jardetzky, 2004), which results in widespread HN–N shift changes from direct and indirect effects for all TM residues (Figure 2B). Further analysis of Hα, 15N, 13Cα and 13C′ backbone chemical shifts (Cornilescu et al, 1999) and HN–HN NOEs confirms that backbone secondary structures are indeed indistinguishable between monomeric and heterodimeric states (Supplementary Figure 3 and Table I). To reliably define the heterodimerization interface, extensive use of selective methyl labelling (Tugarinov and Kay, 2003) was necessary to identify close αIIb–β3 interproton distances, while suppressing the otherwise dominating intrasubunit NOE signals. Including the αIIb(R995)–β3(D723) salt bridge verified here by mutagenesis, 27 intersubunit distance restraints were thus unambiguously identified (Supplementary Figure 4), yielding appropriate coordinate precisions of 0.68 Å for the backbone‐heavy atoms of the ensemble of 20 calculated simulated annealing structures (Figure 5A; Supplementary Table II). The salt bridge may also be excluded without adverse effect on the dimer structure, which independently juxtaposes αIIb(R995) and β3(D723) (Figure 5E and F). Residual dipolar couplings for the heterodimeric state could be measured with only limited accuracy, which negated their inclusion in the structure calculations.
Structure of the αIIbβ3 TM complex and structure‐based mutagenesis
The αIIb and β3 TM helices commence in close proximity at the extracellular membrane border, with close side chain distances detectable (Figure 5C) in agreement with previous disulfide cross‐linking studies in the native receptor (Luo et al, 2004). Guided by packing interactions with three distinct glycine residues, αIIb(G972), αIIb(G976) and β3(G708), the TM helices cross within their N‐terminal halves at an angle of 25±3° (Figure 5B–D). This and the differing length of the αIIbβ3 TM helices would result in a loss of interhelical contacts C‐terminal to β3(L712) on the intracellular side (Figure 5E). Such a loss is apparently compensated by the placement of αIIb(F992‐F993) between the TM helices, which results from the distinct αIIb backbone reversal C‐terminal to its TM helix (Figure 5E and F). The aromatic rings of αIIb(F992‐F993) are in proximity to that of β3(W715), and the hydrophobic assembly is augmented by contacts between β3(I719) and αIIb(F992‐F993) as well as the hydrophobic moiety of αIIb(R995)'s side chain (Figure 5E and F; Supplementary Figure 4A). This assembly enables the strong electrostatic attractions detected by mutagenesis between αIIb(R995) and β3(D723) (Figure 2C) within the relatively low dielectric environment of lipid headgroups, particularly compared with aqueous solution (Ulmer et al, 2001). Thus, integrin αIIbβ3 forms a TM dimer of unique structural complexity.
On the basis of the structure of the αIIbβ3 TM complex, two association elements are differentiated: an outer membrane association motif or clasp (OMC) characterized by packing interactions centred on αIIb(G972), αIIb(G976) and β3(G708) (Figure 5C and D), and an inner membrane association motif or clasp (IMC) based on the hydrophobic αIIb(F992‐F993) and electrostatic αIIb(R995)–β3(D723) bridges (Figure 5E and F). It is noted that the IMC differs from a clasp that was defined earlier based on reported α‐helical conformations for the αIIb(G991‐F992‐F993) motif (Vinogradova et al, 2002). The pivotal nature of the OMC and IMC residues is corroborated by the strongly activating, that is TM complex dissociating, nature of any of the αIIb(G972L), αIIb(G976L), β3(G708I/L), αIIb(F992A), αIIb(F993A), αIIb(R995D) and β3(D723R) point mutations in native receptors (Hughes et al, 1996; Luo et al, 2005; Partridge et al, 2005). Furthermore, these residues are highly conserved among human integrin α and β TM segments (Figure 1). A less strongly activating point mutation, αIIb(T981I/L) (Luo et al, 2005; Partridge et al, 2005), is also found peripheral to the dimer interface where newly introduced Ile/Leu may compete with native αIIb(L980)–β3(G708) interactions (Figure 5C) and thereby disturb the dimer interface. To learn more about the dimer interface, structure‐based site‐directed mutagenesis was performed in integrin αIIb and β3 TM constructs (Figure 6A) and their association in mammalian CHO cell membranes was evaluated. Reduced TM association was achieved by overpacking the OMC relative to the wild type by αIIb(G972S) and αIIb(G976A), but not by αIIb(G972A) (Figure 6B), in good agreement with the TM helix periodicities (Figure 5C and D). These substitutions, taken from other integrin TM segments (Figure 1), raise the possibility of an α–β TM affinity modulation by the OMC. It is also explicitly noted that not all occurring sequence variations have effects, for example, β3(I693A) underpacking at the extracellular membrane border is without consequence (Figure 6B). In addition to αIIb(F992A) or αIIb(F993A) (Hughes et al, 1996), destabilization of the IMC by underpacking was observed for β3(L712A), β3(W715Y) and β3(I719A), but not for αIIb(V990A) in excellent agreement with the complex structure (Figure 5E and F). Thus, two dominant integrin TM association motifs are discerned (IMC and OMC), and mutagenesis suggests that the α–β TM affinity of integrins, most notably the OMC, may vary among different subunit combinations.
Lipid embedding of the αIIbβ3 complex
In addition to the αIIbβ3 complex structure, information about its lipid embedding is required to define the mechanism of integrin TM signalling. Protection from paramagnetic Mn2+EDDA2− present in the aqueous phase was quantified to examine the embedding of the αIIbβ3 complex in its bicelle lipid environment (Altenbach et al, 1994; Lee et al, 2008; Lau et al, 2008b) in comparison to the dissociated subunits. Protection between monomeric and heterodimeric states is quite similar overall (Figure 7A and B), excluding any large changes in lipid association on TM dissociation such as repartitioning the hydrophobic segments C‐terminal to αIIb(K989) or β3(K716) on the intracellular side. This similarity agrees well with backbone conformations that are independent of the αIIbβ3 association state, and the αIIb protection pattern nicely illustrates the αIIb(G991‐F992‐F993) backbone reversal and lipid re‐immersion of the two phenylalanine side chains in both monomeric and heterodimeric states. Compared with monomeric αIIb, the heterodimeric αIIb state showed a detectable increase in protection at the N‐terminal TM helix side and a decrease in protection C‐terminal to the TM helix (V990‐G991). At the intracellular β3 TM helix terminus, an increase in protection is noted for the heterodimeric state (Figure 7B). These changes are compatible with small αIIbβ3 rearrangements relative to the bicelle lipids, and Figure 7C provides an estimate of integrin αIIbβ3 membrane embedding. The interhelical crossing angle in the αIIbβ3 complex suggests a straight αIIb helix and a β3 helix tilt of 25° in accordance with their differing TM helix length. At this point, it is noted that, in the absence of lipid environments, helical conformations for the αIIb(G991‐F992‐F993) sequence, which is fully conserved among all 18 integrin α subunits (Figure 1), were reported (Vinogradova et al, 2002; Weljie et al, 2002). In the absence of the unique environment created by the lipid tail‐to‐headgroup‐to‐solvent transition (Wiener and White, 1992), however, these structures may not be of physiological relevance. In conclusion, the structures, lengths and protection patterns of the integrin αIIb/β3 TM helices indicate an unusual straight/tilted combination in the membrane that is independent of their association state as is their backbone conformation.
Mechanism of integrin αIIbβ3 TM signalling
On the intracellular side, activating ligands can directly disrupt the IMC, which extends into the lipid headgroups (Figure 7C). For example, the activating talin F3 domain is likely to interfere with the IMC (Wegener et al, 2007). In fact, the unusual, asymmetric structure of the αIIbβ3 TM complex may relate to its openness to interference from cytosolic ligands and, compared with a purely helical coiled‐coil‐like assembly, offers additional structural elements amenable to regulatory intervention. The membrane re‐immersion of αIIb(F992‐F993) not only aids in juxtaposing αIIb(R995)–β3(D723), but also makes this central constraint readily accessible (Figure 7C). The highly conserved αIIb(Gly991‐R995) sequence (Figure 1) suggests that this mode of inside‐out activation is general to many integrin receptors. Interestingly, talin also stabilizes the helical propensity of the β tail on exiting the membrane (Ulmer et al, 2001; Li et al, 2002; Wegener et al, 2007), resulting in a stable, elongated helix for the β subunit (Figure 7C). In contrast, on the extracellular side, the agonist‐binding site is far from the extracellular membrane border (c.f. Figure 9) and a direct, enthalpic disruption of the OMC is not possible. The structures of the extracellular domain of integrin αVβ3 and αIIbβ3 (Xiong et al, 2001; Adair et al, 2005; Zhu et al, 2008) show the C‐terminal ends of the α–β ectodomain to be in close proximity (Figure 9B). Therefore, we suggest an indirect, entropic stabilization of the OMC by the associated extracellular lower leg assembly. If such stabilization were present, the weakly αIIbβ3 TM dissociating mutations identified in the absence of the ectodomain (Figure 6B) would be less dissociating in the native receptor. Indeed, all four of the experimentally amenable dissociating mutations were not able to activate native integrin αIIbβ3 in contrast to more disruptive substitutions (Figure 8). Thus, an entropic stabilization of the α–β TM dimer interface by the resting extracellular domains is present and may be lost as a consequence of conformational changes resulting from ligand binding (DiazGonzalez et al, 1996), resulting in outside‐in signalling. By the symmetry of this arrangement, the integrity of the IMC and OMC stabilize the resting conformation of the extracellular domain and disruption of the IMC leads to inside‐out signalling.
In summary, the integrin αIIbβ3 TM complex represents the first structure of a heterodimeric TM receptor and reveals a dimerization interface of intriguing complexity. The IMC stabilizes the integrin TM dimer interface on the intracellular side, the ectodomain and OMC do so on the extracellular side, and the transition between heterodimeric and monomeric TM states proceeds without large rearrangements of αIIbβ3 backbone structure or lipid association. On the basis of these observations, the notion of α–β TM complex dissociation on activation (Hughes et al, 1996; Kim et al, 2003; Li et al, 2005; Zhu et al, 2007), and the available structures of integrin domains, the following refined mechanism of integrin αIIbβ3 TM signalling is proposed. The resting state, with associated TM helices, is stabilized by the packing of C‐terminal residues of the integrin ectodomain, as observed in the resting integrin αVβ3 and αIIbβ3 ectodomain structures (Xiong et al, 2001; Adair et al, 2005; Zhu et al, 2008), and the here described TM dimer interface (Figure 9B). Outside‐in signalling is induced by the separation of the extracellular lower leg assembly (Xiao et al, 2004), after ectodomain interactions with agonists. This results in the loss of entropic stabilization of the TM complex, shifting the equilibrium to the dissociated state (Figure 9C) and transmitting a signal into the cell. For the extracellular domains, a transition from bent to extended conformations is depicted (Xiao et al, 2004; Zhu et al, 2008), but it is noted that alternative rearrangements have been also proposed (Arnaout et al, 2005; Rocco et al, 2008; Ye et al, 2008). Inside‐out signalling is achieved by the direct disruption of the IMC by activating intracellular ligands such as talin, as suggested by cytosolic β tail–talin F3 structures (Figure 7C) (Garcia‐Alvarez et al, 2003; Wegener et al, 2007). The enthalpic disruption of the IMC by talin leads to the collapse of the TM dimer interface, which destabilizes the ectodomain lower leg assembly and allows the extracellular domains to rearrange into high‐affinity conformations (Figure 9A). Thus, we explain integrin αIIbβ3 bi‐directional signalling by the unique structure of its TM complex, its ectodomain conformation‐dependent stabilization and intracellular ligand‐dependent structural interferences.
Materials and methods
NMR sample preparation
Peptides encompassing human integrin αIIb(A958‐P998) and β3(P685‐F727), including β3(C687S), respectively, were produced as described earlier (Lau et al, 2008a, 2008b). In addition, a peptide incorporating αIIb(R995A) was produced analogously. Peptides were produced in four different isotope‐labelling patterns: fully protonated, unlabelled (12C/14N) peptide; partially and highly deuterated, 13C/15N labelled peptide synthesized in 50 and 99% D2O solutions, respectively, using 1H/13C d‐glucose/15N NH4Cl; and selectively Val‐γ1,2 (13CH3/12CD3), Leu‐δ1,2 (13CH3/12CD3), Ile‐δ1 (13CH3)‐labelled peptides within a perdeuterated background in combination with 13C/15N labelling synthesized by supplying the sodium salts of 2‐keto‐3‐methyl‐d3‐butyric acid‐1,2,3,4‐13C4,3‐d1 and 2‐ketobutyric acid‐13C4,3,3‐d2 (Tugarinov and Kay, 2003), and 2H/13C D‐glucose/15N NH4Cl in 99% D2O solution. For HN‐detected experiments, the peptides were typically reconstituted at concentrations of 0.6 and 0.9 mM for 2H/13C/15N‐labelled and unlabelled subunits, respectively, in 385 mM 1,2‐dihexanoyl‐sn‐glycero‐3‐phosphocholine, 83 mM 1‐palmitoyl‐2‐oleoyl‐sn‐glycero‐3‐phosphocholine, 41 mM 1‐palmitoyl‐2‐oleoyl‐sn‐glycero‐3‐[phospho‐l‐serine]. For HC‐detected experiments, both peptides were reconstituted at concentrations of 1.2 mM in deuterated lipids, 350 mM 1,2‐dihexanoyl(d22)‐sn‐glycero‐3‐phosphocholine‐1,1,2,2‐d4‐N,N,N‐trimethyl‐d9, 105 mM 1,2‐dimyristoyl‐d54‐sn‐glycerol‐3‐phosphocholine‐1,1,2,2‐d4‐N,N,N‐trimethyl‐d9. These samples were prepared in 25 mM HEPES·NaOH, pH 7.4, 6% D2O, 0.02% w/v NaN3 solutions and, if desired, freeze dried and exchanged into D2O. To measure residual dipolar couplings, the peptides were dissolved at concentrations of 0.3 mM and 0.4 mM for 2H/13C/15N‐labelled and unlabelled subunits, respectively, in 25 mM KH2PO4/K2HPO4, pH 7.4, 75 mM KCl containing 1,2‐dihexanoyl‐sn‐glycero‐3‐phosphocholine and 1‐palmitoyl‐2‐oleoyl‐sn‐glycero‐3‐phosphocholine at concentrations of 100/30 mM or 200/60 mM and G‐tetrad liquid crystals formed from 25 mg/ml d(GpG) (Lorieau et al, 2008).
NMR spectroscopy and structure calculation
All NMR experiments were conducted on a cryoprobe‐equipped Bruker Avance 700 spectrometer. Data were processed and analysed with the nmrPipe package (Delaglio et al, 1995) and CARA. Pulse sequences were applied with TROSY optimization (Pervushin et al, 1998). Starting from the monomeric αIIb and β3 resonances (Lau et al, 2008a, 2008b), HN, 15N, 13Cα backbone assignments of the heterodimeric set of resonances (Figure 2) were achieved from HSQC, HNCA, NOESY‐TROSY and HSQC‐NOESY‐TROSY experiments using highly deuterated peptide in complex with fully protonated partner. Hα and H/C side chain assignments were achieved from (CT)‐HSQC, HAHB(CBCACO)NH, (H)CCH‐COSY, H(C)CH‐COSY and NOESY‐HSQC experiments (Gehring and Ekiel, 1998) using partially deuterated, 13C/15N‐labelled peptide uncomplexed and in complex with fully protonated partner, respectively. Selectively, Val‐γ1,2 (13CH3/12CD3), Leu‐δ1,2 (13CH3/12CD3), Ile‐δ1 (13CH3)‐labelled peptides uncomplexed and in complex with fully protonated partner, respectively, were assigned by (H)CCC(CO)NH, H(C)CC(CO)NH and NOESY‐HSQC experiments (Grzesiek et al, 1993). Spectral overlap was resolved and NOE intensities were optimized by recording experiments at different temperatures (23, 28 and 33 °C) and using different mixing times (75, 100 and 125 ms). H–N residual dipolar couplings were measured from 1JNH‐scaled HNCO experiments (Kontaxis et al, 2000).
Backbone torsion angle restraints were derived from TALOS‐based database searches (Cornilescu et al, 1999) using 1Hα, 15N, 13Cα and 13C′ chemical shifts. HN–HN distance constraints were obtained from 15N‐edited NOESY experiments. To reliably detect interhelical NOEs selective methyl labelling was indispensable and from 13Cmethyl–1H, 13C‐edited NOESY‐HSQC experiments and the herein verified αIIb(R995)–β3(D723) salt bridge (Figure 2C), 27 unambiguous distance restraints were obtained. Representative NOE strips are provided in Supplementary Figure 4. Because of the complex relationship of individual NOE amplitudes and interproton distances in noncovalently associated complexes (Campbell and Sykes, 1993) and ensuing referencing ambiguities, only upper distance bounds were defined at ⩽5.5 Å for the detected methyl NOE connectivities, in analogy to protocols that do not require lower distance bounds (Kuszewski et al, 1999). Limited accuracy of the measured residual dipolar couplings negated their inclusion in the structure calculations. The structure of the αIIbβ3 TM complex was calculated by simulated annealing, starting at 3000 K, using the XPLOR‐NIH program (Schwieters et al, 2003). In addition to standard force field terms for covalent geometry (bonds, angles and improper dihedrals) and nonbonded contacts (Van der Waals repulsion), dihedral angle and interproton distance restraints were implemented using quadratic square‐well potentials, and a backbone–backbone hydrogen‐bonding potential and torsion angle potential of mean force were used (Kuszewski et al, 1997; Grishaev and Bax, 2004). The final values for the force constants of the different terms in the simulated annealing target function are as follows: 1000 kcal mol−1 Å−2 for bond lengths; 500 kcal mol−1 rad−2 for angles and improper dihedrals, which serve to maintain planarity and chirality; 4 kcal mol−1 Å−4 for the quartic Van der Waals repulsion term; 30 kcal mol−1 Å−2 for interproton distance restraints; 200 kcal mol−1 rad−2 for dihedral angle restraints; 1.0 for the torsion angle potential; and a directional force of 0.20 and a linearity force of 0.05 for the hydrogen‐bonding potential. Appropriate convergence for all 20 calculated structures to coordinate precisions of 0.68 and 1.05 Å relative to the mean coordinates was obtained for the backbone‐heavy and all nonhydrogen atoms, respectively (Supplementary Table II). Moreover, the calculated structural ensemble is insensitive to the random removal of 10% of intermolecular distance restraints (data not shown). Structural statistics are summarized in Supplementary Table II. The atomic coordinates have been deposited in the Protein Data Bank with the accession number 2K9J.
Affinity capture of αIIb™‐TAP/Tac‐β3™ constructs
For the construction of αIIbTM‐TAP (see Figure 6A), the sequences of the preprotrypsin leader sequence followed by three FLAG repeats (Sigma‐Aldrich, Inc.) were cloned into pcDNA3.1 (Invitrogen, Inc.). Subsequently, PCR‐generated fusion sequences coding for αIIb(Gln954‐Glu1008) and TAP were ligated into the vector. Tac‐β3TM (see Figure 6A) was generated by the ligation of PCR‐generated fusion sequences coding for the extracellular Tac domain and β3(Val681‐Thr762) into pcDNA3.1. Point mutations were performed using the Quick‐change site‐directed mutagenesis kit (Stratagene, Inc).
At 24 h after co‐transfection of pcDNA3.1/αIIb™‐TAP and pcDNA3.1/Tac‐β3™, CHO cells were lysed with CHAPS lysis buffer (20 mM HEPES, pH 7.4, 1% CHAPS, 150 mM NaCl, 2 mM CaCl2, Roche EDTA‐free protease inhibitor mixture) and were clarified by centrifugation at 14 000 rpm for 15 min. The clarified lysates were incubated with calmodulin sepharose (GE Healthcare, Inc.) for 2 h at 4 °C, and bound proteins were eluted with SDS reducing sample buffer, subjected to SDS–PAGE and analysed by western blotting.
Activation assay of functional integrin αIIbβ3
Flow cytometric activation assays were performed as described earlier (Feral et al, 2005; Han et al, 2006). In brief, αIIb and β3 subunits bearing point mutations in the TM segment (Figure 8) were co‐transfected into CHO cells. At 24 h after transfection, cells were stained with PAC1 (an activation‐specific αIIb–β3 antibody) to measure activation, and with D57 (an αIIb–β3 complex‐specific antibody) to measure surface expression, in the presence and absence of the integrin‐activating Mn2+ cation. After washing, cells were stained with fluorescein isothiocyanate‐conjugated anti‐mouse IgG and with R‐phycoerythrin‐conjugated anti‐mouse IgM. Five minutes before analysis, propidium iodide (PI) was added, and PI‐negative live cells were analysed on FACSCalibur (BD Biosciences). Data were analysed using WinMDI version 2.9 to generate dot plots (Supplementary Figure 5).
Supplementary data are available at The EMBO Journal Online (http://www.embojournal.org).
We thank Diana Gegala for critically reading the manuscript. This work was supported by Grants from the US National Institutes of Health to TSU (HL089726) and MHG (HL70784 and AR27214). TSU is recipient of a Scientist Development Grant from the American Heart Association. Tong‐Lay Lau and Chungho Kim are recipients of postdoctoral fellowships from the American Heart Association. The authors declare no competing financial interests.
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