| Literature DB >> 35155724 |
Marko Popovic1, Marta Popovic2.
Abstract
Since the beginning of the COVID-19 pandemic, SARS-CoV-2 has mutated several times into new strains, with an increased infectivity. Infectivity of SARS-CoV-2 strains depends on binding affinity of the virus to its host cell receptor. In this paper, we quantified the binding affinity using Gibbs energy of binding and analyzed the competition between SARS-CoV-2 strains as an interference phenomenon. Gibbs energies of binding were calculated for several SARS-SoV-2 strains, including Hu-1 (wild type), B.1.1.7 (alpha), B.1.351 (beta), P.1 (Gamma), B.1.36 and B.1.617 (Delta). The least negative Gibbs energy of binding is that of Hu-1 strain, -37.97 kJ/mol. On the other hand, the most negative Gibbs energy of binding is that of the Delta strain, -49.50 kJ/mol. We used the more negative Gibbs energy of binding to explain the increased infectivity of newer SARS-CoV-2 strains compared to the wild type. Gibbs energies of binding was found to decrease chronologically, with appearance of new strains. The ratio of Gibbs energies of binding of mutated strains and wild type was used to define a susceptibility coefficient, which is an indicator of viral interference, where a virus can prevent or partially inhibit infection with another virus.Entities:
Keywords: COVID-19; Gibbs energy of binding; SARS CoV-2 delta strain; SARS-CoV-2 threat; Virus-virus-host interactions
Year: 2022 PMID: 35155724 PMCID: PMC8816792 DOI: 10.1016/j.mran.2022.100202
Source DB: PubMed Journal: Microb Risk Anal ISSN: 2352-3522
Gibbs energy of binding of SARS-CoV-2 strains. The values of the binding constant, K, and Gibbs energy of binding, Δ, values were calculated using K values from the literature. Mutations led to increase in binding affinity and decrease in Gibbs energy of binding, implying greater spontaneity of binding of mutated strains. More negative Gibbs energy makes the process of antigen-receptor binding more favorable. The values have been calculated at 37⁰C (310.15 K).
| Date of isolation | PANGO lineage | WHO label | First outbreak | Mutations | KD (M) | Reference | KB ( | ΔbG (kJ/mol) |
|---|---|---|---|---|---|---|---|---|
| Dec-19 | Hu-1 | Wild type | Wuhan | Wild type | 2.13E-08 | 4.69E+07 | −45.55 | |
| Dec-19 | Hu-1 | Wild type | Wuhan | Wild type | 4.03E-07 | 2.48E+06 | −37.97 | |
| 26-Jan-21 | B.1.1.7 | Alpha | United Kingdom | 8.76E-08 | 1.14E+07 | −41.90 | ||
| May-20 | B.1.351 | Beta | South Africa | 2.04E-07 | 4.90E+06 | −39.72 | ||
| May-20 | B.1.351 and P.1 | Beta and Gamma | South Africa and Brazil | E484K | 1.97E-08 | 5.08E+07 | −45.75 | |
| B.1.36 | / | India, Canada, and UK | N440K | 9.90E-09 | 1.01E+08 | −47.53 | ||
| 10/1/2020 | B.1.617 | Delta | India | L452R/E484Q | 4.60E-09 | 2.17E+08 | −49.50 | |
| Dec-19 | Hu-1 | Wild type | Wuhan | WT | 6.26E-08 | 1.60E+07 | −42.77 | |
| 18-Dec-20 | B.1.1.7 | Alpha | United Kingdom | N501Y (Alpha) | 5.5E-09 | 1.82E+08 | −49.04 | |
| 26-Jan-21 | B.1.1.7 | Alpha | United Kingdom | E484K/N501Y (UK2) | 3.7E-09 | 2.70E+08 | −50.06 | |
| 14-Jan-21 | B.1.351 | Beta | South Africa | K417N | 3.49E-07 | 2.87E+06 | −38.34 | |
| 14-Jan-21 | B.1.351 | Beta | South Africa | K417N/E484K | 2.51E-07 | 3.98E+06 | −39.19 | |
| 14-Jan-21 | B.1.351 | Beta | South Africa | K417N/E484K/N501Y (Beta) | 1.74E-08 | 5.75E+07 | −46.07 | |
| Nov-20 | P.1 | Gamma | Brazil | K417T | 2.26E-07 | 4.42E+06 | −39.46 | |
| Nov-20 | P.1 | Gamma | Brazil | K417T/E484K | 1.47E-07 | 6.80E+06 | −40.57 | |
| Nov-20 | P.1 | Gamma | Brazil | K417T/E484K/N501Y (Gamma) | 1.22E-08 | 8.20E+07 | −46.99 | |
Fig. 1.Evolution of Gibbs energy of binding and susceptibility coefficient of SARS-CoV-2. (a) The SARS-CoV-2 mutant strains are characterized by a more negative Gibbs energy of binding compared to the wild type. (b) The susceptibility coefficient has been increasing with new mutations on the SARS-CoV-2 virus.