| Literature DB >> 34094257 |
Rajeev Ramanan1, Shobhit S Chaturvedi1, Nicolai Lehnert2, Christopher J Schofield3, Tatyana G Karabencheva-Christova1, Christo Z Christov1.
Abstract
The N ε-methylEntities:
Year: 2020 PMID: 34094257 PMCID: PMC8162366 DOI: 10.1039/d0sc03713c
Source DB: PubMed Journal: Chem Sci ISSN: 2041-6520 Impact factor: 9.825
Scheme 1N ε-Lysine methylation and demethylation of histone H3 play important roles in the regulation of transcription.
Fig. 1Outline of catalytic cycle for the JmjC KDMs.
Fig. 3Distances between the dioxygen derived proximal oxygen (Op) to the substrate N-methyl N (Op–N) (in red) and of the distal oxygen (Od) to the 2OG co-substrate (C2–Od) (in black) during the 1 μs simulation. The x-axis denotes time in ns, and the y-axis denotes distance in Å. Atom labels are shown in the inset.
Fig. 2Views of the KDM4A·Fe(iii)·O2-substrate (H3(7–12)K9me3) complex. (a) Geometry of the optimized ferric-superoxo [Fe(iii)–O2] complex for KDM4A. (b) The quantum mechanical region used in calculations. Wiggly lines define the boundary of the QM/MM partition. The views were derived from a modeled structure of Fe(iii)–O2 complexed with H3(7–12)K9me3 (based PDB: 2OQ6) as described in Methods.
Fig. 4Motions in the Fe(iii)–O2·2OG H3(7–12)K9me3 complex. (a) Dynamic cross-correlation diagram with important correlations circled. Residues 158–170 belong to α5 and β6; 227–234 belong to α7. (b) Principal component analysis showing the direction of motions yellow to blue.
Fig. 5Substrate dynamics for the Fe(iv)-oxo intermediate. (a) Fe(iv)-oxo intermediate with the substrate and MO diagram for a σ-trajectory HAT. (b) Distance of the Fe(iv)-oxo O to substrate N during the 1 μs simulation. The y-axis is distance (Å) and x-axis is time (ns). (c) Variation in the Fe–O–N angle for the 1 μs simulations. The y-axis is the angle (°).
Fig. 6Influence of protein dynamics on catalysis and overview of the whole catalytic events. (a) The QM(B1)/MM optimized TS geometry. (b) Potential energy profile (in kcal mol−1) for HAT and the rebound step at the QM(B2)/MM followed by QM(B2+ZPE)/MM level of theory. The inset shows the barrier for multiple HAT events at the QM(B2+ZPE)/MM level with starting geometry of the corresponding IM2. Distances are in Å; angles in degrees (°). (c) Superimposed geometries of the optimized reactants for the KDM4A·Fe(iv)-oxo·H3(7–12)K9me3 complex. (d) Spin Natural Orbitals (SNO) of HAT transition state with populations in parentheses. (e) Summary of important steps in the catalytic cycle with QM(B2+ZPE)/MM energies in kcal mol−1.
Fig. 7KDM4A mutation causes changes in substrate orientation from productive to non-productive. (a) The first geometry of simulation for the (grey) variants is overlapped with the geometry at 1000 ns (blue for Tyr177Ala; green for Lys241Ala; red for Asn290Ala). (b) Distances for the Fe(iv)O to substrate Nε of wildtype and KDM4A variants. y-Axis: distance in Å; x-axis: time in ns. Colors: black for WT; blue for Tyr177Ala; green for Lys241Ala; red for Asn290Ala.
Fig. 8Comparisons of binding interactions in CP2(R6Kme3) with those for H3(7–12)K9me3. (a) Binding of the cyclic peptide (CP2(R6Kme3)) to KDM4A. (b) The distance of the O of the FeO intermediate to the N of the substrate N-methyl group during 1 μs simulation for H3(7–12)K9me3 (black) and CP2(R6Kme3) (red). The y-axis is labeled with distance in Å and x-axis with time in ns. (c) Representation of Fe–O–N angle for H3(7–12)K9me3 (black) and CP2(R6Kme3) (red). y-Axis: angle in degrees (°).
Fig. 9Influence of protein dynamics on the barrier in the CP2(R6Kme3) bound KDM4A. (a) Potential energy profile for HAT and rebound step for CP2(R6Kme3) substrate/inhibitor at the QM(B2)/MM followed by QM(B2+ZPE)/MM level of theory. (b) The barrier for multiple HAT at the QM(B2+ZPE)/MM level of theory with starting geometric details of the corresponding IM2. Barriers are in kcal mol−1, distances in Å and angles in degrees (°).