CONFORMATIONS OF SILICON-CONTAINING RINGS PART 1 - A CONFORMATIONAL STUDY ON 1,3,5-TRISILACYCLOHEXANE - COMPARISON OF AB-INITIO, SEMIEMPIRICAL, AND MOLECULAR MECHANICS CALCULATIONS - CONFORMATIONAL ENERGY SURFACE OF 1,3,5-TRISILACYCLOHEXANE
I. Arnason et al., CONFORMATIONS OF SILICON-CONTAINING RINGS PART 1 - A CONFORMATIONAL STUDY ON 1,3,5-TRISILACYCLOHEXANE - COMPARISON OF AB-INITIO, SEMIEMPIRICAL, AND MOLECULAR MECHANICS CALCULATIONS - CONFORMATIONAL ENERGY SURFACE OF 1,3,5-TRISILACYCLOHEXANE, Journal of molecular structure. Theochem, 454(1), 1998, pp. 91-102
The structure and relative energies for the basic conformations of 1,3
,5-trisilacyclohexane (1) have been calculated by several methods and
their performance compared. It is found that HF ab initio calculations
using the basis set 6-31G, the SV(P) basis set used by TURBOMOLE and
the MM3 force field produce mutually fairly consistent results. MM2 p
erforms not as well as MM3, but in many cases MM2 performs better than
3-21G. Three semiempirical methods (AM1, MNDO, and PM3) were tested.
None of them was found to produce reliable results. It is found by ab
initio (6-31G and SV(P)) and MM3 calculations that the dihedral angle
s for the chair conformation are 52.7-53.1 degrees, which makes (1) mo
re flattened than cyclohexane, and thus (1) does not exhibit behaviour
similar to cyclohexasilane, which is less flattened than cyclohexane.
The ring flattening of (1) is mainly caused by the intrinsically larg
e SiCSi bond angle (114.1-114.8 degrees). The twist conformation of (1
) is found by the same calculations to be 2.1-3.1 kcal mol(-1) higher
in energy than the chair conformation, and the boat form is found to b
e 0.3-0.4 kcal mol(-1) higher than the twist form. These values are mu
ch closer to the values for cyclohexasilane than to those for cyclohex
ane. The conformational energy surface of (1) has been calculated by u
sing MM3. The energy barrier from the chair to the twist conformation
of (1) is found to be 5.5 kcal mol(-1) (C) 1998 Elsevier Science B.V.
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