| Literature DB >> 34206274 |
Anwar Mohammad1, Fahd Al-Mulla2, Dong-Qing Wei3, Jehad Abubaker1.
Abstract
SARS-CoV-2Entities:
Keywords: RNA dependent RNA polymerase; Remdesivir; SARS-CoV-2; molecular dynamic simulations
Mesh:
Substances:
Year: 2021 PMID: 34206274 PMCID: PMC8301449 DOI: 10.3390/biom11070919
Source DB: PubMed Journal: Biomolecules ISSN: 2218-273X
Figure 1(The structure RdRp (PDB ID: 7BV2) [22]. (A) Viral RNA template entry and the NTP entries are shown with black arrowheads, the route for the release of RNA template and product after replication are shown with a black arrow and two dashed black arrows. The NiRAN, b-hairpin, palm fingers, and interface are part of nsp12, nsp8 is depicted in orange and nsp7 in red. The A97V and P332L mutations are depicted in blue. (B) Chemical structure and 3D conformer of Remdesivir (RDV).
Figure 2The H-bonding network or RDV interacting with RdRp residues in (A) WT, (B) A97V, and (C) P323L structures.
Figure 3RMSD plots of 200-ns molecular dynamic simulations of RdRp in apo and complex with RDV. (A) WT−apo and A97V−apo, (B) WT−apo and P323L, (C) WT−RDV and A97V−RDV complex (D) WT−RDV and P323L−RDV complex.
Figure 4RMSF plot of 200-ns simulations of RdRp in apo and complex with RDV. Apo WT, A97V and P323L RdRp (A) and WT-RDV, A97V-RDV complex and (B) P323L-RDV complex.
Free energy of all the systems are calculated in kcal/mol.
| Systems | vdW | Elec | SASA | GTotal (ΔG) |
|---|---|---|---|---|
| Wild Type | −27.2 | 21.8 | −3.6 | −17.3 |
| A97V complex | −20.3 | −9.6 | −2.6 | −14.4 |
| P323L complex | −36.9 | −2.2 | −4.2 | −24.1 |
Figure 5Principal component analyses (PCA) were plotted against each other; Apo WT, A97V and P323L RdRp and WT-RD, A97V-RDV and P33L-RDV RdRp complex.
Figure 6The covariance matrix constructed from the whole MD trajectory fraction of motion of the first 10 eigenvectors plotted against the corresponding eigenvector. The first 10 eigenmodes were used to calculate the percentage fraction of motion of each eigenvector for RdRp-apo (A) and RdRp-RDV (C), and the fraction of motions by a single eigenvector for RdRp-apo (B) and RdRp-RDV complex (D).
Tabulated individual eigonvector contribtions.
| Eigenvectors | WT-Apo | A97V-Apo | P323L-Apo | WT-RDV | A97V-RDV | P323L-RDV |
|---|---|---|---|---|---|---|
| EV 1 | 37.62 | 27.7 | 38.4 | 39.944 | 39.462 | 13.564 |
| EV 2 | 15.43 | 17.37 | 19.17 | 14.726 | 15.838 | 11.77 |
| EV 3 | 14.09 | 12.68 | 11.45 | 9.705 | 10.257 | 11.101 |
| EV 4 | 8.27 | 10.01 | 6.77 | 8.148 | 9.385 | 10.457 |
| EV 5 | 6.31 | 7.81 | 6.12 | 6.486 | 6.95 | 9.952 |
| EV 6 | 4.79 | 6.78 | 4.93 | 5.866 | 5.344 | 9.595 |
| EV 7 | 4.27 | 5.92 | 4.35 | 5.116 | 3.891 | 8.941 |
| EV 8 | 3.78 | 4.26 | 3.65 | 3.896 | 3.376 | 8.681 |
| EV 9 | 3.01 | 3.91 | 2.73 | 3.398 | 2.964 | 8.324 |
| EV 10 | 2.43 | 3.57 | 2.43 | 2.716 | 2.535 | 7.616 |
Figure 7Free energy landscape (FEL) is represented as a function of PC1 and PC2. Projections of motions in the phase space at 300 K of RdRp WT−apo, A97V−apo, P323 L−apo, WT−RdV, A97V−RDV, P323L−RDV are shown. The first and second PC modes from the PCA of the backbone carbon atom fluctuations were used.