| Literature DB >> 35479875 |
Duc Tuan Cao1, Thi Mai Huong Doan2,3, Van Cuong Pham2,3, Thi Hong Minh Le2, Jung-Woo Chae4, Hwi-Yeol Yun4, Min-Kyun Na4, Young-Ho Kim4, Minh Quan Pham3,5, Van Hung Nguyen1.
Abstract
Heat shock protein 90 (Hsp90) is one of the most potential targets in cancer therapy. We have demonstrated using a combination of molecular docking and fast pulling of ligand (FPL) simulations that marine fungi derivatives can be possible inhibitors, preventing the biological activity of Hsp90. The computational approaches were validated and compared with previous experiments. Based on the benchmark of available inhibitors of Hsp90, the GOLD docking package using the ChemPLP scoring function was found to be superior over both Autodock Vina and Autodock4 in the preliminary estimation of the ligand-binding affinity and binding pose with the Pearson correlation, R = -0.62. Moreover, FPL calculations were also indicated as a suitable approach to refine docking simulations with a correlation coefficient with the experimental data of R = -0.81. Therefore, the binding affinity of marine fungi derivatives to Hsp90 was evaluated. Docking and FPL calculations suggest that five compounds including 23, 40, 46, 48, and 52 are highly potent inhibitors for Hsp90. The obtained results enhance cancer therapy research. This journal is © The Royal Society of Chemistry.Entities:
Year: 2021 PMID: 35479875 PMCID: PMC9033662 DOI: 10.1039/d1ra01855h
Source DB: PubMed Journal: RSC Adv ISSN: 2046-2069 Impact factor: 4.036
Fig. 1Computational modelling of molecular docking and FPL simulations.
The obtained values of the docking simulations
| No. | PDB ID | Δ | Δ | Δ | Δ | Δ | ChemPLP | Δ |
|---|---|---|---|---|---|---|---|---|
| 1 |
| −10.2 | −8.8 | −8.8 | −8.8 | −8.8 | 74.7 | −8.91 |
| 2 |
| −9.6 | −8.7 | −9.2 | −10.4 | −7.0 | 66.4 | −7.85 |
| 3 |
| −10.2 | −9.9 | −9.4 | −10.0 | −7.9 | 75.2 | −7.41 |
| 4 |
| −8.3 | −7.7 | −7.9 | −8.1 | −7.3 | 68.3 | −10.98 |
| 5 |
| −9.2 | −8.2 | −8.2 | −8.2 | −7.9 | 61.4 | −9.91 |
| 6 | 3 R4M | −7.8 | −6.6 | −6.6 | −7.5 | −5.1 | 49.7 | −8.13 |
| 7 |
| −8.3 | −7.1 | −7.4 | −7.6 | −5.4 | 61.2 | −9.45 |
| 8 |
| −10.1 | −8.8 | −8.7 | −9.2 | −6.0 | 73.2 | −11.19 |
| 9 |
| −9.6 | −8.2 | −8.2 | −8.2 | −6.4 | 70.5 | −10.33 |
| 10 |
| −11.3 | −10.0 | −9.9 | −10.6 | −11.8 | 98.9 | −11.53 |
| 11 |
| −10.7 | −9.7 | −9.8 | −10.0 | −11.8 | 98.3 | −11.70 |
| 12 |
| −12.5 | −11.5 | −11.4 | −11.5 | −11.4 | 96.4 | −10.20 |
| 13 |
| −12.5 | −11.9 | −11.9 | −12.0 | −11.5 | 95.5 | −10.13 |
| 14 |
| −11.6 | −10.7 | −10.7 | −10.8 | −11.0 | 93.8 | −10.57 |
| 15 |
| −12.3 | −11.5 | −11.7 | −11.7 | −11.1 | 94.2 | −11.39 |
The experimental binding free energy was obtained through the inhibition constant. The unit of energy and force are in kcal mol−1 and pN, respectively.
Fig. 2Association between the ChemPLP score and the experimental binding free energy ΔGEXP.
The obtained values of the FPL calculations in comparison with the respective experiments
| No. | Name |
|
| Δ |
|---|---|---|---|---|
| 1 |
| 580.7 ± 90.9 | 67.7 ± 12.3 | −8.91 |
| 2 |
| 764.3 ± 119.3 | 76.5 ± 12.9 | −7.85 |
| 3 |
| 676.2 ± 78.5 | 71.1 ± 8.7 | −7.41 |
| 4 |
| 1065.5 ± 66.3 | 113.9 ± 10 | −10.98 |
| 5 |
| 831.4 ± 52.5 | 82.7 ± 4.5 | −9.91 |
| 6 | 3 R4M | 605.7 ± 81.7 | 58.3 ± 9.4 | −8.13 |
| 7 |
| 651.0 ± 37.6 | 69.8 ± 4.4 | −9.45 |
| 8 |
| 1140.8 ± 128.1 | 126.3 ± 17.2 | −11.19 |
| 9 |
| 910.8 ± 88.1 | 98.8 ± 8.6 | −10.33 |
| 10 |
| 1357.1 ± 146.7 | 167.6 ± 28 | −11.53 |
| 11 |
| 1566.1 ± 124.2 | 208.5 ± 26.1 | −11.70 |
| 12 |
| 1313.2 ± 88.2 | 164.4 ± 20.3 | −10.20 |
| 13 |
| 1363.3 ± 131.0 | 175.7 ± 25.9 | −10.13 |
| 14 |
| 1348.6 ± 102.6 | 163.9 ± 18.6 | −10.57 |
| 15 |
| 1318.9 ± 112.6 | 157.5 ± 20.8 | −11.39 |
The obtained value of the mean rupture force FMax.
The recorded metric of the pulling work W.
The experimental binding free energy ΔGEXP was estimated via the reported ki. The calculated error was the standard error of the average. The unit of force and energy is in pN and kcal mol−1, respectively.
Fig. 3Association between the average of the FMax and the experimental binding free energy ΔGEXP.
The obtained values of the molecular docking and FPL calculations
| No. | Name | ChemPLP |
|
| Δ |
|
|---|---|---|---|---|---|---|
| 1 | 48 | 86.3 | 627 ± 127.1 | 70.6 ± 9.2 | −8.62 | 0.29 |
| 2 | 25 | 77.8 | 555.3 ± 60.5 | 61.7 ± 8.2 | −8.38 | 1.25 |
| 3 | 40 | 76.9 | 711.7 ± 77.9 | 75.7 ± 13 | −8.90 | 0.54 |
| 4 | 23 | 72.6 | 827.6 ± 195 | 95.9 ± 22.3 | −9.29 | 0.67 |
| 5 | 46 | 71.7 | 669.9 ± 97.2 | 78.1 ± 9.8 | −8.76 | 0.85 |
| 6 | 52 | 70.6 | 753.3 ± 110 | 77.5 ± 10.5 | −9.04 | 0.43 |
The obtained value of the mean rupture force FMax.
The recorded metric of the pulling work W.
The predicted binding free energy ΔGPreFPL was estimated using formula (1). The calculated error was the standard error of the average. The unit of force, energy, and inhibition constant are pN, kcal mol−1 and μM, respectively.
Fig. 4The 6 binding positions of the marine fungi compounds docking the best to Hsp90, which were estimated using the GOLD docking program with ChemPLP scoring function.