| Literature DB >> 29184081 |
Jiao Chen1,2, Jie Yang1,2, Xianqiang Sun3,4, Zhongming Wang1,2, Xiaolan Cheng1,2, Wuguang Lu1,2, Xueting Cai1,2, Chunping Hu1,2, Xu Shen1, Peng Cao5,6.
Abstract
Neomorphic mutation R140Q in the metabolic enzyme isocitrate dehydrogenase 2 (IDH2) is found to be a driver mutation in cancers. Recent studies revealed that allosteric inhibitors could selectively inhibit IDH2/R140Q and induce differentiation of TF-1 erythroleukemia and primary human AML cells. However, the allosteric inhibition mechanism is not very clear. Here, we report the results from computational studies that AGI-6780 binds tightly with the divalent cation binding helices at the homodimer interface and prevents the transition of IDH2/R140Q homodimer to a closed conformation that is required for catalysis, resulting in the decrease of the binding free energy of NADPHs. If the allosteric inhibitor is removed, the original open catalytic center of IDH2/R140Q will gradually reorganize to a quasi-closed conformation and the enzymatic activity might recover. Unlike IDH2/R140Q, AGI-6780 locks one monomer of the wild-type IDH2 in an inactive open conformation and the other in a half-closed conformation, which can be used to explain the selectivity of AGI-6780. Our results suggest that conformational changes are the primary contributors to the inhibitory potency of the allosteric inhibitor. Our study will also facilitate the understanding of the inhibitory and selective mechanisms of AG-221 (a promising allosteric inhibitor that has been approved by FDA) for mutant IDH2.Entities:
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Year: 2017 PMID: 29184081 PMCID: PMC5705638 DOI: 10.1038/s41598-017-16427-w
Source DB: PubMed Journal: Sci Rep ISSN: 2045-2322 Impact factor: 4.996
Figure 1AGI-6780 binds in an allosteric manner at the dimer interface of IDH2/R140Q. The detailed interaction mode is shown in the right panel.
Figure 2Molecular dynamics (MD) simulations of IDH2/R140Q_αKG and IDH2/R140Q_AGI-6780 systems. (A) Evolution of RMSDs during 400 ns MD simulation. (B) The active site entrance of IDH2/R140Q. The residues of I116, F148 and L289 are colored purple and cyan respectively in the structures of IDH2/R140Q_αKG (green) and IDH2/R140Q_AGI-6780 (yellow). (C) Evolution of the Cα distances of Ile116-Leu289′ and angles of Ile116-Phe148-Leu289′ in monomer A and B during MD simulation. D and E represent the probability distributions of Cα distances of Ile116-Leu289′ and angles of Ile116-Phe148-Leu289′. F and G represent the surface maps around the catalytic center of IDH2/R140Q_αKG and IDH2/R140Q_AGI-6780 respectively.
The calculated binding free energy and reDock scores of NADPHs with IDH2/R140Q in the presence/absence of AGI-6780.
| Systems | NADPH | Binding free energy (kcal/mol) | reDock Score |
|---|---|---|---|
| IDH2/R140Q_AGI6780 | NADPHA | −509.75 | −12.99 |
| NADPHB | −646.63 | −12.60 | |
| IDH2/R140Q_αKG | NADPHA | −1418.89 | −20.60 |
| NADPHB | −1382.28 | −19.10 |
The Cα distances of Ile116-Leu289′ and angles of Ile116-Phe148-Leu289′.
| System | Distance | Angle | ||
|---|---|---|---|---|
| I116A-289B (Å) | I116B-L289A (Å) | I116A-F148A-L289B (°) | I116B-F148B-L289A (°) | |
| IDH2/R140Q_AGI6780a | 22.24 | 20.37 | 61.10 | 56.30 |
| IDH2/R140Q_AGI6780b | 22.01 ± 0.96 | 19.34 ± 0.97 | 60.77 ± 2.56 | 54.43 ± 2.98 |
| IDH2/R140Qb | 14.62 ± 0.68 | 17.95 ± 0.85 | 40.34 ± 2.05 | 48.66 ± 2.24 |
| IDH2/R140Q_αKGc | 12.54 | 12.54 | 34.40 | 34.40 |
| IDH2/R140Q_αKGb | 14.04 ± 0.33 | 14.95 ± 1.07 | 37.41 ± 1.01 | 40.56 ± 2.98 |
| IDH2/R140QQ316A_AGI6780b | 20.52 ± 0.76 | 18.24 ± 0.77 | 55.76 ± 2.28 | 49.45 ± 2.33 |
| WT_AGI6780b | 18.04 ± 0.70 | 22.75 ± 1.43 | 49.59 ± 1.81 | 62.08 ± 3.64 |
aCrystal structure of IDH2/R140Q_AGI6780 (PDB: 4JA8); bMD simulation systems, the average distances and angles were calculated from the 300–400 ns trajectory; cCrystal structure of IDH2/R140Q_αKG (PDB: 5I95).
Figure 3Structural superposition of IDH2/R140Q_AGI-6780 (open conformation, colored yellow) and IDH2/R140Q_αKG (closed conformation, colored green) after 400 ns MD simulation.
Figure 4RMSD matrices of IDH2/R140Q_AGI-6780 (A) and IDH2/R140Q (B) systems during MD simulation.
Figure 5(A) The direction of motion between IDH2/R140Q_AGI-6780 (yellow) and IDH2/R140QQ316A_AGI-6780 (cyan) after 400 ns simulation. (B) Detailed interaction mode of AGI-6780 with IDH2/R140QQ316A. (C) Evolution of the Cα distances of Ile116-Leu289′ and angles of Ile116-Phe148-Leu289′ in the system of IDH2/R140QQ316A_AGI-6780 during MD simulation.
The binding free energy (MM/GBSA) of AGI-6780 with different IDH2 systems.
| Systems | IDH2/R140Q_AGI-6780 | IDH2/R140QQ316A_AGI-6780 | IDH2/WT_AGI-6780 |
|---|---|---|---|
| MM/GBSA (kcal/mol) | −62.37 ± 3.07 | −47.08 ± 2.75 | −62.25 ± 3.26 |
Figure 6(A) The direction of motion between IDH2/R140Q_AGI-6780 (yellow) and IDH2/WT_AGI-6780 (pink) after 400 ns simulation. (B) Detailed interaction mode of AGI-6780 with IDH2/WT. (C) Evolution of the Cα distances of Ile116-Leu289′ and angles of Ile116-Phe148-Leu289′ in the system of IDH2/WT_AGI-6780 during MD simulation.