Abstract
The nucleotide-binding and oligomerization domain (NOD)-containing protein 1 (NOD1) plays the pivotal role in host-pathogen interface of innate immunity and triggers immune signalling pathways for the maturation and release of pro-inflammatory cytokines. Upon the recognition of iE-DAP, NOD1 self-oligomerizes in an ATP-dependent fashion and interacts with adaptor molecule receptor-interacting protein 2 (RIP2) for the propagation of innate immune signalling and initiation of pro-inflammatory immune responses. This interaction (mediated by NOD1 and RIP2) helps in transmitting the downstream signals for the activation of NF-κB signalling pathway, and has been arbitrated by respective caspase-recruitment domains (CARDs). The so-called CARD-CARD interaction still remained contradictory due to inconsistent results. Henceforth, to understand the mode and the nature of the interaction, structural bioinformatics approaches were employed. MD simulation of modelled 1:1 heterodimeric complexes revealed that the type-Ia interface of NOD1CARD and the type-Ib interface of RIP2CARD might be the suitable interfaces for the said interaction. Moreover, we perceived three dynamically stable heterotrimeric complexes with an NOD1:RIP2 ratio of 1:2 (two numbers) and 2:1. Out of which, in the first trimeric complex, a type-I NOD1-RIP2 heterodimer was found interacting with an RIP2CARD using their type-IIa and IIIa interfaces. However, in the second and third heterotrimer, we observed type-I homodimers of NOD1 and RIP2 CARDs were interacting individually with RIP2CARD and NOD1CARD (in type-II and type-III interface), respectively. Overall, this study provides structural and dynamic insights into the NOD1-RIP2 oligomer formation, which will be crucial in understanding the molecular basis of NOD1-mediated CARD-CARD interaction in higher and lower eukaryotes.
Introduction
Innate immunity plays a crucial role in host-defence mechanism against infectious pathogens, which is governed by a set of germ-line encoded receptors, called as pattern recognition receptors (PRRs) [1]. PRRs are generally activated by invading pathogenic patterns; termed as pathogen-associated molecular patterns (PAMPs) and/or self-generated danger signals, called as damage/danger-associated molecular patterns (DAMPs) [2,3]. These PRRs are classified into five major groups on the basis of their sub-cellular location, domain architecture, structural fold, specificity to ligands and molecular function. Among the five major groups; i.e., Toll-like receptors (TLRs) and C-type lectin receptors (CLRs) are membrane bound, whereas, NOD-like receptors (NLRs), RIG-I-like receptors (RLRs) and AIM2-like receptors (ALRs) are intra-cytoplasmic in nature [4].
Till date, a total of 22 numbers of NLRs have been reported in human and are grouped into five different sub-families based on their N-terminal domain distributions i.e., NLRA, NLRB, NLRC, NLRP and NLRX [5]. The NLR family members show tripartite domain architecture and are characterized by the presence of central nucleotide-binding and oligomerization domain (NOD/NACHT; found in NAIP, CIITA, HET-E and TP1 proteins). In addition to NACHT, they also contain one/two effector-binding domain/s [EBD: CAspase Recruitment Domain (CARD)/ PYrin Domain (PYD)] towards the N-terminal end and a varied number of Leucine Rich Repeats (LRRs) towards the C-terminal region [6–8].
NOD1 is one of the well-characterized receptors in NLRC sub-group and plays a pivotal role in host-defence mechanism. It is activated by recognizing iE-DAP (γ-ᴅ-Glu-meso-diaminopamelic acid, a bacterial peptidoglycan (PGN)), which in turn, triggers nuclear factor-kappa B (NF-κB) signalling [9]. The ligand recognition leads to the activation of the receptor and that causes its conformational alteration, where LRR unfolds from NACHT. Subsequently, the NACHT domain self-oligomerize in ATP-dependent fashion (an unexplored hypothesis), which aid in the transmission of signal(s) to adaptor molecule RIP2 (receptor-interacting serine/threonine protein kinase 2), through CARD-CARD interaction for the subsequent activation of NF-κB signalling cascade and maturation and release of pro-inflammatory cytokines [10]. The dysregulation of NOD1 gene is associated with a number of inflammatory diseases. It has been noticed that certain SNPs (single nucleotide polymorphisms) in NOD1 gene are associated with inflammatory bowel’s disease (IBD), eczema and atopic asthma [11, 12]. For instances, the non-synonymous variant rs2075820 (E266K) in NOD1 gene is associated with increased risk to peptic ulcer patients upon Helicobacter pylori infection [13] and rs2709800 is associated with gastric lesions [14].
The well-studied interaction partner of NOD1 (and NOD2) is RIP2, which helps in transmitting the danger signal(s) for the activation of NF-κB and MAPK signalling pathway. Over last decade, significant efforts have been made by several groups for the exploration of the exact binding patches/interfaces responsible for NOD1- (even NOD2-) mediated CARD-CARD interaction [15–20]. Multiple groups have proposed multiple modes of interactions that include; surface charge interaction, acidic-basic surface interaction and multiple interface interactions [15–20]. However, the elucidation of the interaction modes and binding interfaces of CARDs (of NOD1 and RIP2) has still remained inconclusive. Therefore, in this study, an attempt has been made through a combinational approach involving protein-protein docking followed by multiple molecular dynamics (MD) simulation to delineate the most probable interaction modes, binding interfaces and critical residues involved in NOD1-mediated CARD-CARD interaction. Overall, this study will help in understanding the structural and dynamic features of CARD-CARD interaction, which is expected to stimulate the NOD1-mediated signalling mechanism in a broader perspective.
Computational Methods
Data retrieval and calculation of electrostatic surface potential
The amino acid sequences of NOD1 (NP_006083) and RIP2 (NP_003812) were retrieved from NCBI protein database and the experimentally solved 3D structures of NOD1CARD (PDB ID: 2DBD) and RIP2CARD (2N7Z) [21] were retrieved from PDB (https://www.rcsb.org). The sequence alignments were performed using ClustalX [22]. The binding sites were obtained from APAF1-CASP9 (Ap1-C9) CARD-CARD interfaces (PDB ID: 3YGS [23], 4RHW [24]) and NOD1-RIP2 [15, 19] interaction studies. The electrostatic surface potential of NOD1 and RIP2 CARDs were calculated using Adaptive Poisson-Boltzmann Solver (APBS) [25] with a grid spacing of 0.4 Å, salt concentration of 0.15 M and temperature of 296 K. The dielectric constants were set to ε = 2 for protein and ε = 78 for the solvent.
Modelling of dimeric and trimeric complexes
In order to obtain the possible interaction modes governed by CARDs of NOD1 and RIP2, we performed several docking calculations using PyMOL (superimposition protocol). Primarily, two CARD-CARD complexes were created in reference to Ap1-C9 heterodimer complex (3YGS [23]); where, in complex-I, we superimposed NOD1CARD with Ap1CARD and RIP2CARD with C9CARD (where helix-α1 and α4 of RIP2CARD (basic surface; type-Ia) were found facing to the helix-α2 and α3 (acidic surface; type-Ib) of NOD1CARD); however in complex-II, both NOD1 and RIP2 CARDs were superimposed with C9 and Ap1 CARDs, respectively (i.e., in reverse order of complex-I) (S1A and S1B Fig). Secondly, to perceive the type-II and III interaction interfaces, we docked a monomer (either NOD1 or, RIP2 CARD) (considering the Ap1-C9 heterotrimer complex (S1C Fig); 4RHW [24]) in the third position of stable complex that resulted from MD simulation (see ‘Results and Discussion‘ section) (S1D and S1E Fig). Here, in the trimeric complexes, NOD1 and RIP2 CARDs were superimposed with C9 and Ap1 CARDs in first and second position and in the third position, either an NOD1 and/or RIP2CARD was superimposed with second Ap1CARD (S1F Fig). In addition, we also modelled two type-I homodimers of NOD1CARD and RIP2CARD in reference to CASP1CARD type-I dimeric conformation (5FNA) [26].
Molecular dynamics simulation
In order to explore the dynamic features of individual CARDs of NOD1 and RIP2, and their modelled complexes; MD simulations were performed in GROMACS 4.5.5 [27] simulation suite using Amber99sb-ILDN force field [28] in periodic boundary conditions. The individual CARD structures and modelled complexes were solvated with TIP3P water models within individual cubic boxes. A minimum distance of 10-12Å was retained between protein surfaces and box-edge. Each simulation system was neutralized by adding a physiological strength (0.15M) of counter ions (Na+ and Cl-). Steepest descent energy minimization was performed until a tolerance of 1000 kJ mol-1 to remove steric conflicts between atoms and to avoid high-energy interaction. The energy minimized systems were position-restrained for 1 nanosecond (ns) in two different phases’ viz., NVT (constant volume) and NPT (constant temperature). The final production runs for individual CARDs and docked complexes were carried out for 50ns and 60ns for type-I dimeric and trimeric complexes, respectively. In this study, for each complex [heterodimeric and -trimeric (NOD1-RIP2-RIP2: complex-I and NOD1-RIP2-RIP2: complex-II)], three independent production runs were performed for better sampling of results. Moreover, MD simulation of homodimers (of NOD1/RIP2 CARDs) was performed for 50ns to delineate the existence/stability of type-I homodimer. The atomic compositions of all simulation systems were summarised in S1 Table.
Analysis of MD trajectories
The trajectory analysis was performed using the integrated modules of GROMACS and VMD 1.9.2 [29]. To gauge the dynamic stability, the backbone root mean square deviation (RMSD) and radius of gyration (Rg) of individual CARDs, as well as CARD-CARD complexes, were analysed using g_rmsdist and g_gyrate tools, respectively. The g_hbond tool was used to calculate the total numbers H-bonds that formed between counter CARDs during the course of simulation time. The most widely used method, principal component analysis (PCA) was performed to observe the most relevant and/or correlated motions from the MD trajectories [30], by creating the covariance matrix of main chain atoms of the complexes using g_covar tool. To understand the global motion of CARD complexes (either by structurally or, in phase space), we analysed and projected the fast two principal components (PC1 and PC2) using g_anaieg tool. The g_dist and g_mindist tools were used for calculating interatomic and inter-residual dynamic distances of the intermolecular interactions; those formed between CARD counterparts during the course of the simulation. Molecular visualizations and interaction analysis were performed using PyMOL (academic license) and DIMPLOT (integrated in LigPlot+ v1.4.5; academic license) [31, 32]. The 2D graphs were generated by Grace 5.1.25 program (http://plasma-gate.weizmann.ac.il/Grace/).
Results and Discussion
Structural stability and electrostatic surface potential of individual CARDs
The dynamic stability and compactness of CARDs were gauged by calculating the backbone RMSD and Rg from the MD trajectories. The backbone RMSD and Rg were found to be stable in both the CARDs as displayed in Fig 1A. The solved NOD1CARD (2DBD) showed six numbers of closely packed α-helices; however, in RIP2CARD (2N7Z) 6th helix position was proposed to be a coil [21]. The analysis of secondary structure from MD trajectory seemed quite stable during the simulation period and a 310-helix cum turn was noticed in the α6 position of RIP2CARD (Fig 1B). Though the structural fold of both CARDs was found to be alike, the calculated electrostatic surface potential exhibited differential surface charge distribution. NOD1CARD showed an extensive negative surface and a small positively charged patch; however, RIP2CARD portrayed several positive and negative patches over the surface (Fig 1B and 1C). Owing to the interest of this study, two potential type-I surface patches (both positive (α1 and α4; type-Ia) and negative (α2 and α3; type-Ib)) were identified on the basis of earlier reports on NOD1/NOD2-RIP2 and Ap1-C9 CARD-CARD interaction [15–20,23,24,33,34]. The binding patches including the critical/surface exposed residues (experimentally proved/predicted) were illustrated in Fig 1C–1E.
Interaction types, critical residues and molecular docking
The electrostatic component is the basis of CARD-CARD interaction. An observation based on Ap1-C9 complex (3YGS and 4RHW) solicits that acidic surface (helix-α2 and α3; type-Ib) of Ap1CARD and basic surface (α1 and α4; type-Ia) of C9CARD are indispensable type-I interface [23,24]. However, a recent observation revealed that type-I and type-II interfaces were necessary for Ap1-C9 interaction (4RHW) and a type-III interaction mode was noticed in the same complex between two Ap1CARD, which is crucial for apoptosome activity [24]. So far, Ap1-C9 (4RHW) and RIG-I-MAVS (4P4H) are two solved heterotrimeric CARD-CARD complexes, which clearly describe all three interface types (type-I, II, and III) [24,35].
Over the last decade, different mutational studies and the sequence-structure analysis has revealed that two possible binding patches i.e., either basic (α1 and α4) and/or acidic (α2 and α3) are crucial for NOD1/2-RIP2-mediated CARD-CARD interaction [15–18]. According to Manon et al. [15] an acidic surface (E53, D54, and E56) of NOD1CARD and basic surface (R444, R483, and R488) of RIP2CARD were essential for NOD1-RIP2 interaction, and the findings were well supported by Boyle and co-workers [18]. Conversely, in the same experiment [15], it was also reported that ‘R69E’ mutation (from basic surface) reduced the interaction ability of NOD1CARD with RIP2CARD. In contrast, Fridh and Rittinger [17] proposed that the acidic surface of RIP2CARD (D461, E472, E475, and D492) might be essential for NOD1-RIP2 interaction. However, a recent report on NOD1-RIP2 interaction proposed that a single interface (either basic or, acidic surface of NOD1CARD/RIP2CARD) might be insufficient for signal transmission [19]. Therefore, a total of four CARD-CARD complexes were prepared (S1 Fig; see ‘Computational Methods‘ section) and optimized through MD simulation.
Type-Ia interface of NOD1CARD is essential for 1:1 interaction
Analysis of complex stability
In order to identify the probable NOD1-RIP2 CARD-CARD dimer, we inferred the stability and compactness of the complexes by calculating the backbone RMSD and Rg; and performed PCA to detect the list-motioned CARD-CARD complexes. The RMSD and Rg graphs from three individual trajectories (S1, S2, and S3) retained a stable backbone deviation and compactness in complex-II; however, in complex-I, unstable backbone deviation, and gyradius were noticed (Fig 2A). Similarly, the comparative PCA results revealed that complex-I showed a higher eigenvalue and occupied a larger area in phase space; whereas, complex-II covered a smaller area and showed distinct clusters (Fig 2B). Moreover, the visual inspection to the dynamic motion of the complexes indicated a higher motion in complex-I than in complex II (Fig 2B).
H-bond analysis
H-bonding is one of the major intermolecular forces that govern the binding stability of the protein and its partner(s). For the better understanding of the binding stability and nature of interaction, we analysed the intermolecular H-bonds (between CARDs of NOD1 and RIP2) of heterodimeric complexes as a function of simulation time. The analysed H-bonds (from all three individual simulations; S1, S2, and S3) in complex-II showed higher numbers of H-bonds and retained a stable H-bonding pattern; however, an unstable pattern and lesser numbers of H-bonds were noticed in complex-I (Fig 2C). Altogether, considering the above observations into account, the complex-II was projected as stable 1:1 NOD1-RIP2 complex for interaction study.
Dynamic interaction analysis (NOD1CARD-RIP2CARD type-I interface)
The results from Manon and co-workers have revealed that E53, D54, and E56 of NOD1CARD (acidic patch) and R444, R483 and R488 (basic patch of RIP2CARD) are crucial for NOD1-mediated CARD-CARD interaction; however, in the same experiment, the group proposed a charge reversal mutation (R69E in NOD1CARD) abrogated the downstream signalling [15]. In another study, Fridh and Rittinger [17] proposed that the mutations, D461A, E472A, E475A and D492A (acidic patch of RIP2CARD) disrupt NOD1-RIP2 interaction. Moreover, Mayle et al. anticipated the critical role of Y474 (of RIP2CARD type-Ib patch) in NOD1-mediated CARD-CARD interaction [19]. In the present study, the final snapshots from all three stable individual productions runs (S1, S2, and S3 of complex-II) were considered as representative structures to perceive the detailed intermolecular interactions between NOD1CARD and RIP2CARD. The interaction analysis of all three individual snapshots (observed by DIMPLOT [31]) showed an average of 7–8 numbers of H-bonds (S2 Fig). The residues, K24, E28 and R69 of NOD1CARD, and D461, R466, D467 and K508 of RIP2CARD were found to be involved in H-bonding. In addition to H-bonds, all other possible interactions were considered for dynamic interaction calculation as shown in Fig 3A. Further, to observe the consistency and stability in intermolecular interactions driven by NOD1 and RIP2 CARDs, the interatomic and inter-residual distances were calculated. The distance calculation result revealed six numbers of dynamic H-bonds (which include two strong salt bridges, R69-D461 and E28-R466 and two H-bonds, K24-D461, and E28-K508) (Fig 3A; left panel). In addition to H-bonds, we also noticed five electrostatic interactions (N26-S465; R27-S465; E28-D461; E28-S465; R69-Y474) and eight hydrophobic contacts between K24, S25, R27, E28, V31 and R69 (of NOD1CARD), and N457, D461, A462 and S465 (of RIP2CARD) (Fig 3A; right panel). However, the interactions of E472, E475 and D492 (of RIP2CARD; proposed by Fridh and Rittinger [17] couldn’t be established in type-I interface due to altered side chain orientation and position. The presented mode of NOD1-RIP2 CARD-CARD interaction model was found be similar with that of type-I mode of interaction as reported earlier in heterodimeric CARD complexes (Ap1-C9 [23, 24] and RIG-I-MAVS [35]; (Fig 3B)). A close visual inspection to the type-I mode of NOD1-RIP2 interaction (Fig 3B; right panel) partially supports the finding of Manon et al. [15] (on R69’s involvement); Mayle et al. [19] (on the participation of type-Ia surface patch of NOD1CARD and type-Ib interface including ‘Y474’ of RIP2CARD) and Fridh and Rittinger (on D461 of RIP2CARD) [17].
Involvement of multiple interfaces in NOD1-RIP2 interaction
The experimentally solved oligomeric CARD complexes portrayed three different types of interaction, i.e., type-I, II, and III [24, 35]. In a recent study, Mayle et al. suggested that a single interface interaction might be insufficient for signal transduction and proposed the existence of type-I and type-III interface [19]. Additionally, the authors denied the participation of type-Ia interface of RIP2CARD and type-Ib interface of NOD1CARD in NOD1:RIP2 heterodimer formation [19]. Here, we observed that the type-Ia interface of NOD1CARD and type-Ib interface of RIP2CARD might be a suitable interface for NOD1:RIP2 1:1 CARD-CARD interaction, which is consistent to Mayle and co-author’s observation [19]. To perceive the possibility of type-II and III mode of interaction, we modelled two trimeric complexes (complex-I: NOD1-RIP2-NOD1; complex-II: NOD1-RIP2-RIP2) considering Ap1-C9 heterotrimer (4RHW [24]) as the template (see ‘Computational Methods‘ section; S1D–S1F Fig). Further, to determine the dynamic stability of the generated heterotrimeric CARD complexes, MD simulation of individual complexes was performed for 60ns.
Analysis of dynamic stability of the complexes and intermolecular H-bonds
To understand complex stability, we have analysed the backbone RMSD of both the heterotrimeric complexes (complex-I and II) and performed PCA to observe the global motion. The calculated backbone RMSD of complex-II (NOD1-RIP2-RIP2) was found to be stable with a deviation of ~2.15 Å, whereas, an unstable and higher RMSD was perceived in complex-I (Fig 4A). Further, to obtain a list-motioned complex, we analysed the global motion of the complexes structurally as well as in phase space (by analysing the first two principal components: PC1 and PC2). As portrayed in Fig 4B, the scattered plots, and a comparatively larger motion was observed in complex-I; whereas in complex-II, we perceived distinct clusters in the phase space and list flexible complex structures.
Furthermore, to deduce the nature of binding stability, we calculated the total numbers of H-bonds between the monomers (in all three interfaces) as a function of simulation time. The H-bond analysis of type-I (NOD1-RIP2) and type-III interfaces (RIP2-NOD1; complex-I and RIP2-RIP2; complex-II) indicated the interaction stability (S3 Fig); however, in type-II interface, an unusual H-bonding pattern was noticed in complex-I (NOD1-NOD1) (S3A Fig). The superimposed complex structures (before and after MD) suggested a stable structural orientation in complex-II (S3B Fig). But in complex-I, the NOD1CARD (in the third place) showed distorted orientations (S3A Fig), where it can be assumed that the type-II interfaces of NOD1 might be the unsuitable for homo-dimerization. Hence, complex-II (NOD1-RIP2-RIP2) was proposed as the stable heterotrimer.
Dynamic interaction analysis (of type-II and III interface)
To understand the intermolecular interactions governed by NOD1CARD and RIP2CARD in type-II interface and (between two) RIP2 CARDs in type-III interface, the final snapshot from each individual run (S1, S2, and S3) were considered as representative structures for interaction study. The interaction analysis of three snapshots was performed using DIMPLOT program (S4A and S4B Fig) and the conserved interaction pairs (Fig 4C and 4D) was taken for dynamic interaction analysis by calculating their interatomic/inter-residual distances. The interatomic/inter-residual distance graphs (of NOD1-RIP2 type-II interface) revealed ten hydrophobic contacts; four electrostatic interactions and two H-bonds (governed by D73 of NOD1CARD and R483 of RIP2CARD (Fig 4C)). Moreover, we also noticed some electrostatic interactions between D48, Y49, S77 and K78 of NOD1CARD and T452, R483 and K513 of RIP2CARD and several hydrophobic contacts between Y49, S77, K78, G79, E81 and V82 (of NOD1CARD) and N449, Q450, T452, Q514, M515, G516 (of RIP2CARD). Out of the interacting residues proposed for the type-II interface, only R483 was anticipated by Manon et al. [15] to be involved in the NOD1-RIP2 interaction. In type-III interface (between two RIP2 CARDs), the interaction was found to be dominated by H-bonds and electrostatic components (Fig 4D). The distance calculation revealed that E472 and E475 (of type-IIIa interface), and R483 and R488 of type-IIIb interface of RIP2CARD were involved in H-bonding. Further, we also noticed that K471 and T479 (type-IIIa) formed electrostatic interaction and hydrophobic contacts with N449, P481, T482 and T484 (type-IIIb) (Fig 4D).
The proposed model of NOD1-RIP2-RIP2 heterotrimer complex was found similar to that of Ap1-C9 [24] and RIG-I-MAVS [35] trimeric conformations (Fig 5A). As illustrated in Fig 5B, the detailed tri-faced (NOD1-RIP2-RIP2) mode of interaction revealed ‘inter-surface/patch’ interaction network. In type-I mode of interaction, the residues K24, N26, R27, E28 and R69 of type-Ia patch (α1 and α4) of NOD1 was found to interact with N457, A462, L464, S465, R466, Y474 and K508 (type-Ib patch) of RIP2CARD (Figs 3B and 5B). Also, it was noticed that D73 of NOD1CARD (despite being present in type-Ia interface) formed strong H-bonds with R483 (type-IIIb patch) of RIP2CARD and the interactions were found dynamically stable in all three trajectories (Fig 4C). It can be speculated that the inter-patch interaction (D73-R483) might be playing some important role in the signal transmission which needs experimental validation in the near future.
NOD1 and RIP2 CARDs form type-I homodimer in heterotrimeric conformation
Manon et al. [15] and Mayle et al. [19] suggested the possibility of type-I homodimer in RIP2CARD and Ver Heul et al. [36] revealed the helix-swapped homodimer of NOD1 (S5A Fig). After analysing the type-I electrostatic interfaces of NOD1 and RIP2 CARDs, we assumed the existence of the plausible type-I homodimer in NOD1 and RIP2 CARDs. To infer the dynamic existence of type-I homodimers, we modelled NOD1 and RIP2 homodimeric CARD complexes (see ‘Computational Methods‘ section) (S5B Fig) and performed a 50ns MD simulation. The dynamic stability, compactness, and the nature of interactions were analysed by calculating the backbone RMSD, Rg and intermolecular H-bonds as a function of simulation time. The resulting RMSD and Rg of homodimeric complexes indicated a stable backbone deviation and gyradius after 35ns of simulation time (S5C Fig). H-bond analysis revealed a conserved bonding pattern in NOD1CARD dimer; whereas in case of RIP2, an unstable bonding pattern and lesser H-bonds (2.422) were noticed (S5D Fig). The superimposition of pre and post-MD structures indicated a tilted orientation of dimers (S5E Fig). Henceforth, to perceive the existence of type-I homodimers in heterotrimeric complex; the monomers of RIP2 and NOD1 CARD were docked individually to modelled type-I homodimers of RIP2CARD and NOD1CARD in reference to Ap1-C9 heterotrimer, as a result two other heterotrimeric complexes were created (NOD1-NOD1-RIP2: complex-III and RIP2-RIP2-NOD1: complex-IV)(4RHW [24]; S6A Fig). Thereafter, the modelled complexes were subjected to 50ns MD simulation to delineate their complex stability. To perceive the dynamic stability and the nature of the interaction, we analysed the backbone RMSD and Rg, and calculated the intermolecular H-bonds in all the interfaces. In complex-III, we noticed a stable backbone deviation and gyradius; while in complex-IV, a higher RMSD was observed after 33ns (S6B Fig). The calculated H-bonds (as a function of simulation time) and structural superimposition of heterotrimers (pre and post-MD) indicated lower RMS (2.495Å) and stable H-bonding pattern in complex-III (S6C Fig); whereas in complex-IV, we observed a higher RMS (4.445Å) and fewer H-bonds in type-III interface after 40ns of MD (S6D Fig).
Interaction analysis (type-I interfaces)
The interaction analysis of representative structures extracted from the trajectory (10ns interval) revealed a conserved interaction pattern in all the interfaces (S7 and S8 Figs). In the NOD1 homodimeric interface, we observed a strong salt bridge [between R69 (type-Ia) and D42 (type-Ib)], four electrostatic interactions (S25-K46, R27-D42, E28-N43, R69-Q38) and three hydrophobic contacts (K24-L45/A52, R27-L45) (Fig 6A). However, in RIP2 counterpart, we observed a total of four-five dynamically stable H-bonds (R488-D461, E445-R466, D492-K471), three electrostatic interactions (R444-S465, R488-N457/Y474) and five hydrophobic contacts (Q441/S442-S465, R444-L464, E445-A462, V448-D461) between the type-I interfaces of RIP2CARDs (Fig 6B). Amongst the critical residues predicted to be involved in type-I homodimeric interactions (NOD1/RIP2; this study), D42, N43 and R69 of NOD1CARD and R444, D461, Y478, R483, R488, D492 and D495 of RIP2CARD are the residues that are already reported to be involved in NOD1/NOD2-RIP2 interactions [15, 17, 19].
RIP2CARD might be using its type-IIa interface for NOD1-RIP2 interaction
In first stable heterotrimeric complex (NOD1-RIP2-RIP2 (complex-II)), we observed a type-II mode of interaction between type-IIa interface of NOD1CARD and type-IIb interface of RIP2CARD (Fig 4C) and the similar type of interactions were also observed in complex-III (NOD1-NOD1-RIP2) (S7B Fig). However, in complex-IV (RIP2-RIP2-NOD1), though we observed stable interactions between the type-IIa and type-IIb interfaces of RIP2 and NOD1 CARDs (S8B Fig), which were found to be less in comparison to the type-II mode of interaction, which was observed in the first trimeric complex (NOD1-RIP2-RIP2) (Fig 4C). The second type-II interaction comprised of four H-bonds (including a salt bridge between D492 and R35), one electrostatic interaction (E472-N36) and five hydrophobic contacts (S9 Fig). Additionally, another salt bridge, which was being observed between R35 of NOD1CARD (type-IIb) and E475 (type-IIIa) of second RIP2CARD (S9 Fig; right panel) might be crucial for NOD1-RIP2 signal transmission mechanism.
Type-III interfaces of both the CARDs are dynamically suitable for the interaction
In 2014, Mayle et al. explored the existence of type-III mode of interaction between NOD1 and RIP2 CARDs and proposed that E53 of NOD1CARD (type-IIIa interface) and R483 (type-IIIb interface) of RIP2CARD are crucial for interaction. In the current study, we observed two type-III modes of interactions between NOD1 and RIP2 CARDs. In complex-III, the interactions were noticed between the type-IIIa interface (E53, E56, I57, and A60) of NOD1CARD and the type-IIIb patch (P481, T482, R483, and T484) of RIP2CARD (Fig 7A); however in complex-IV, the crucial residues, E472, E475 and T479 (of the type-IIIa of RIP2CARD) and T63, P65 and R69 (type-IIIb patch of NOD1CARD) showed the interaction (Fig 7B). In addition, an inter-patch interaction (which includes two strong salt bridges) was noticed between ‘R35’ of NOD1CARD and E475 (type-IIIa patch) and D492 (type-Ia interface) of RIP2CARD (S9 Fig, Fig 7B). Of the interacting residues involved in second type-III heterodimeric interface, D492 of RIP2CARD was proposed to be interacting with NOD1 and NOD2 CARDs [17]. The observed residues participating in type-III interface-interactions (this study), were already reported to be trivial (and/or vice versa) [15, 17, 19]. According to Mayle et al. the mutations of solvent exposed residues, D446, V448, T484, S485, K486, Q497 and E522 of RIP2CARD had no role in the interaction with NOD1CARD; however, we noticed the active participation of T484 and Q497 in type-III (Fig 7) and type-II (S9 Fig) interfaces, respectively.
To understand the evolutionary perspective of critical residues involved in multimeric-interface interactions, we performed multiple sequence alignment of individual CARDs of NOD1 and RIP2 of various species and mapped the critical residues involved in intermolecular CARD-CARD interactions (Fig 8). As evident from multiple sequence alignment, the predicted interacting residues from homo/heterodimeric interfaces, R27, E28, V31, Q38, D42, N43, E53, I57, R69, K78, G79 and A96 of NOD1CARD (Fig 8A) and R444, Q450, T452, N457, D461, A462, L464, M470, E472, Y474, E475, L476, T482, R483, T484, R488, D492, K513 and Q514 of RIP2CARD (Fig 8B) were found to be conserved. However, a key residue ‘D73’ of NOD1CARD [involved in inter-patch interaction in the NOD1-RIP2-RIP2 heterotrimeric complex (Fig 7B)] was found to be variable (replaced by ‘E’ in fish species). Particularly, some of the key charged residues, K24 of type-Ia, D48 (also involved in type-I homodimer) and E81 (replaced by ‘Q’ in pufferfish) of type-IIa, and E56 (replaced by ‘D’ in pufferfish) of type-IIIa interface of NOD1CARD, and R466 (replaced by ‘K’ in opossum), D467 and K508 (replaced by ‘R’) of type-Ib interface were found to be variable. Overall, the multiple sequence analysis revealed the existence of residual differences in higher and lower vertebrates, and the paradox in zebrafish [23] might be due to the differential structural orientation of critical type-I interface residues or the residual variation; which needs further experimentation for legitimacy.
Conclusion
In the present study, we employed the structural bioinformatics approaches to irradiate the possible binding interfaces of NOD1 and RIP2 CARDs involved in the so-called CARD-CARD interaction. Our observation suggests the possible existence of NOD1:RIP2 type-I heterodimer and three heterotrimeric complexes with different combinations of NOD1 and RIP2 CARDs. Herein, we noticed that the alternately charged residue (E28 of type-Ia interface of NOD1CARD and R466 of type-Ib interface of RIP2CARD) presumed to contribute to the interaction despite being present in charge reversal patch. Moreover, we detected an inter-patch/surface interaction between type-Ia interface residue ‘D73’ of NOD1CARD and type-IIIb interface residue ‘R483’ of second RIP2CARD in the first (NOD1-RIP2-RIP2) and second (NOD1-NOD1-RIP2) heterotrimeric complexes, which might be critical in transmitting danger signals for the propagation of NF-κB signalling. We also observed the type-I homodimeric existence of NOD1 and RIP2 CARDs in two dynamically stable heterotrimeric complexes, which can be considered as second and third trimeric complexes (probably) responsible for downstream signalling. Altogether, our study demonstrates the molecular basis of NOD1-mediated CARD-CARD interaction, which would open up better avenues to understand the binding interfaces that govern the said interaction. Finally, the amino acids predicted in this study to be involved in the intermolecular interaction warrants further investigation for the legitimacy of this work.
Supporting Information
Acknowledgments
The authors thank Dr. Budheswar Dehury, Scientist-B, RMRC (ICMR), Bhubaneswar (Odisha) for critical reading of the manuscript, and Mr. Ashutosh Vats, Animal Genomic Lab., ABTC, ICAR-NDRI, Karnal (Haryana) for helping in simulation set up during the revision period. We would also like to acknowledge to the esteemed reviewers for their critical comments, which made our manuscript more scientific.
Data Availability
All relevant data are within the paper and its Supporting Information files.
Funding Statement
The authors received no specific funding for this work.
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Supplementary Materials
Data Availability Statement
All relevant data are within the paper and its Supporting Information files.