| Literature DB >> 30274324 |
Ramiro F Quijano-Quiñones1, Carolina S Castro-Segura2, Gonzalo J Mena-Rejón3, Mariana Quesadas-Rojas4, David Cáceres-Castillo5.
Abstract
Mechanistic theoretical studies about the feasibility of the traditional proposed mechanism of formation for icetexane diterpene dimer grandione were assessed using density functional method at the M06-2X/6-31G(d,p) level of theory. Bulk water solvent effects were taken into account implicitly using the polarizable continuum model (SCI-PCM). The results were compared with the selectivity found in the biomimetic synthesis performed by experimental research groups. The relative free energy calculation shows that the one-step H-DA formation mechanism nominated in the literature is not a viable mechanism. We found that an alternative competing Tandem pathway is consistent with the experimental trends. Thus, our results suggested that the compound grandione is formed via a H-DA/retro-Claisen rearrangement and not by the traditional H-DA mechanism proposed early in the experimental studies. The H-DA initial step produce a biecyclic adduct followed by a domino retro-Claisen rearrangement that releases the energy strain of the bicyclic intermediary. Steric issues and hyperconjugation interactions are the mainly factors driving the reaction nature and the selectivity in the formation reaction. Finally, the enzymatic assistance for dimer formation was analyzed in terms of the calculated transition state energy barrier.Entities:
Keywords: DFT; grandione; icetexane dimer; tandem reaction
Mesh:
Substances:
Year: 2018 PMID: 30274324 PMCID: PMC6222908 DOI: 10.3390/molecules23102505
Source DB: PubMed Journal: Molecules ISSN: 1420-3049 Impact factor: 4.411
Figure 1Biosynthetic mechanism for formation of the icetexane dimer grandione proposed in the literature [24,25].
Relative enthalpies, entropies, and Gibbs energies (kcal/mol) for the stationary points involved in the DA reactions at 298.15 K and 1 atm in water.
| Molecule |
|
| |||||||
|---|---|---|---|---|---|---|---|---|---|
| ΔGreac | ΔHreac | TΔSreac | ΔGact | ΔHact | TΔSact | ΔGact | ΔHact | TΔSact | |
| Grandione | −19.07 | −36.31 | −17.24 | 37.31 | 20.85 | −16.45 | - | - | - |
| Grandione β | −19.52 | −38.51 | −18.99 | 40.98 | 22.43 | −18.56 | 44.26 | 25.79 | −18.47 |
| Isograndione | −20.29 | −38.54 | −18.24 | 37.74 | 22.13 | −15.61 | - | - | - |
| Isograndione β | −20.26 | −38.84 | −18.58 | 43.94 | 25.95 | −17.99 | 33.43 | 15.80 | −17.63 |
Figure 2Schematic view of the proposed Tandem mechanism for the formation of isograndione and grandione compounds.
Relative energy Gibbs reactions (kcal/mol) for the stationary points involved in the Tandem reactions at 298.15 K and 1 atm in water.
| Molecule | ΔGact(TS1) | ΔG(INT) | ΔGact(TS2) | ΔGreac |
|---|---|---|---|---|
| Grandione | 21.13 | 7.43 | 13.06 | −19.07 |
| Isograndione | 27.00 | 8.27 | 15.06 | −20.29 |
Figure 3Equilibrium geometries of intermediaries and transition states and their relative energies for the domino process to lead to (a) the isograndione and (b) grandione molecules.
Deformation and interaction energy (kcal/mol) at the TS in grandione and isograndione.
| Molecule |
| TS1 | ||
|---|---|---|---|---|
| ∆ | ∆ | ∆ | ∆ | |
| Grandione | 23.42 | −2.73 | 27.68 | −23.66 |
| Isograndione | 23.90 | −1.84 | 35.61 | −27.66 |
Figure 4Structure of the TS1 (a) and the intermediate (b) and TS2 (c) transition states for the icetexane dimer grandione showing the main interatomic distances.
Figure 5Equilibrium geometries of the endo transition state of grandione β (a) and isograndione β (b) showing an emergent steric repulsion due to the hydroxyl moiety orientation.