The potential energy surface (PES) of 1,3-dioxanes features a number of minima including chair conformers and flexible forms, which are separated by several potential barriers [1][2][3]. However, there are only two minima in the case of 1,3-dioxa-2-silacyclohexanes [4]. In order to evaluate whether this behavior holds for other saturated heterocyclic systems, we used the RHF/3-21G(d) method in the framework of the HyperChem Modeling Program [5] to study the conformational isomerization of 2,2-dimethyl-1,3-dioxa-2-germacyclohexane (1) and compare it with its carbon analog, 2,2-dimethyl-1,3-dioxane (2), which displays ring inversion rapid on the NMR time scale at room temperature [6,7].Our result is similar to the findings for the silicon analogs. The PES of dioxagermacyclohexane 1 contains only two minima corresponding to chair conformers (C and C inv), which are degenerated in energy and separated by 2,5-twist (2,5-T) transition states (TS). The correctness of this assignment for the twist form was confirmed by the finding of one imaginary frequency in the corresponding Hessian. O O Ge Me Me O O Ge Me Me O O Ge Me Me Germacyclohexane 1 (DE, kcal/mol) C (0) C inv (0) 2,5-T (3.6) TSThere are no other minima or transition states in this case. Besides the case of 1,3-dioxa-2-silacyclohexanes [4], such a single-barrier transition to an alternative form has been found previously only for cyclohexane heteroanalogs with an sp 2 atom at the second ring position, in particular, for 2-oxo-1,3-dioxanes [8] and substituted 1,3,2-dioxaborinanes [9, 10].