Optimized geometries and total energies for 3,4‐dihydro‐1,2‐dioxin
(1), 3,6‐dihydro‐1,2‐dioxin (2), 4H‐1,3‐dioxin
(1,3‐diox‐4‐ene, 3), and 2,3‐dihydro‐1,4‐dioxin (1,4‐dioxene,
4) were calculated using ab initio 3‐21G, 6‐31G*, and
MP2/6‐31G*//6‐31G* methods. The half‐chair conformers of 1
(C1), 2 (C2), 3
(C1), and 4 (C2) are more stable
than their respective planar structures [1
(Cs), 2
(C2v), 3
(Cs), and 4
(C2v)]. Among the four isomers
1–4, the half‐chair conformer of 3 is the most
stable. It is 53.1, 54.6, and 3.4 kcal mol−1
more stable than 1, 2, and 4, respectively. The
largest energy difference (19.0 kcal mol−1) is
observed between the half‐chair and planar conformers of 2. The boat
conformers of 2 and 4 are less stable than their respective
half‐chair conformers, but are more stable than their planar structures.
Hyperconjugative orbital interactions (anomeric effects) contribute to the
greater stability of 3(nO(3)
→σ*C(2)—O(1),
nO(3)→σ* C(2)—H ax,n
O(3)→σ* C(2)—H ax
) and of 4 (nO(1)→
σ* C(2)—H ax).
The ab initio calculated structural features of the half‐chair
conformations of the dihydrodioxins 1–4 are compared
with the half‐chair conformations of cyclohexene and the chair
conformations of cyclohexane, oxacyclohexane (tetrahydropyran),
1,2‐dioxacyclohexane (1,2‐dioxane), 1,3‐dioxacyclohexane (1,3‐dioxane), and
1,4‐dioxacyclohexane (1,4‐dioxane) © 1997 by John Wiley &
Sons, Inc. J Comput Chem 18: 1392–1406, 1997