The anomeric and reverse anomeric effect. A simple energy decomposition model for acetals and protonated acetals
Geometry optimizations at the 6-31G** level were performed on various conformers of XH m CH 2 YH n and XH m CH 2 YH n+I + (protonated), with X, Y = N, O. The resulting anomeric stabilization energies were decomposed into steric, electrostatic (lone pair - lone pair, lone pair - hydrogen), and electr...
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Veröffentlicht in: | Canadian journal of chemistry 1992-05, Vol.70 (5), p.1562-1572 |
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Hauptverfasser: | , |
Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | Geometry optimizations at the 6-31G** level were performed on various conformers of XH
m
CH
2
YH
n
and XH
m
CH
2
YH
n+I
+
(protonated), with X, Y = N, O. The resulting anomeric stabilization energies were decomposed into steric, electrostatic (lone pair - lone pair, lone pair - hydrogen), and electronic contributions. Using approximate values for steric and electrostatic terms, the electronic energy was determined to be about −2 kcal/mol for the anomeric effect to arise from O, and −2.5 kcal/mol if it arises from N. For protonated systems, an additional energy term for the reverse anomeric effect had to be added, having a value of −4 kcal/mol for O in OH-CH
2
-NH
3
+
and −5 kcal/mol for N in NH
2
C-H
2
-NH
3
+
. The anomeric effect due to N drives NH
2
-CH
2
-OH
2
+
to a charge-dipole complex of the type NH
2
=CH
2
+
... OH
2
. The energy parameters obtained have been applied to predict relative stabilities of various conformers of methanetriol, aminomethanediol, and protonated methanetriol, with good success. |
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ISSN: | 0008-4042 1480-3291 |
DOI: | 10.1139/v92-192 |