| Literature DB >> 36115608 |
Fangfang Yan1, Feng Gao2.
Abstract
Entities:
Year: 2022 PMID: 36115608 PMCID: PMC9475024 DOI: 10.1016/j.jinf.2022.09.011
Source DB: PubMed Journal: J Infect ISSN: 0163-4453 Impact factor: 38.637
Fig. 1Dynamic cross-correlation matrices and porcupine plots of RBDs. Correlation of residues in RBDs of: (A) original SARS-CoV-2, (B) alpha, (C) beta, (D) gamma, (E) delta and (F) omicron variants. Correlated and anti-correlated movements between residues are shown in red and green, respectively. Comparison of movement strength and direction of residues between the original SARS-CoV-2 and (G) alpha, (H) beta, (I) gamma, (J) delta and (K-L) omicron variants. All plots are constructed based on the first eigenvector and eigenvalues obtained from the diagonalization of the covariance matrix, the length and direction of the purple arrows indicate the movement strength and direction of residues, respectively.
Fig. 2Evaluation of the binding affinity of the original, alpha, beta, gamma, delta and omicron RBDs to ACE2 by MM-PBSA, and residues on RBDs that have important influence on the binding of different SARS-CoV-2 strains to ACE2. (A) Each term of the binding free energy, including total binding free energy (), van der Waals interaction (), electrostatic interaction (), polar solvation free energy (), non-polar solvation free energy () and the superposition () of and . (B) Residues with significant energy contribution to RBD-ACE2 binding, and the residues that are favorable and unfavorable for RBD-ACE2 binding are shown in pink and blue, respectively. Residues that are more affected by mutation are marked with a yellow “★”. (C) Detailed energy changes of residues that are key contributors to the differences in receptor-binding ability between the mutant and original SARS-CoV-2 strains. All values are in kcal/mol.