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. 2013 Aug;19(8):3015-26.
doi: 10.1007/s00894-013-1835-7. Epub 2013 Apr 10.

DFT studies of the conversion of four mesylate esters during reaction with ammonia

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DFT studies of the conversion of four mesylate esters during reaction with ammonia

Andrzej Nowacki et al. J Mol Model. 2013 Aug.

Abstract

The energetics of the Menshutkin-like reaction between four mesylate derivatives and ammonia have been computed using B3LYP functional with the 6-31+G** basis set. Additionally, MPW1K/6-31+G** level calculations were carried out to estimate activation barrier heights in the gas phase. Solvent effect corrections were computed using PCM/B3LYP/6-31+G** level. The conversion of the reactant complexes into ion pairs is accompanied by a strong energy decrease in the gas phase and in all solvents. The ion pairs are stabilized with two strong hydrogen bonds in the gas phase. The bifurcation at C2 causes a significant activation barrier increase. Also, bifurcation at C5 leads to noticeable barrier height differentiation. Both B3LYP/6-31+G** and MPW1K/6-31+G** activation barriers suggest the reaction 2 (2a + NH3) to be the fastest in the gas phase. The reaction 4 is the slowest one in all environments.

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Figures

Figure
Figure
Ammonium salt formation in a Menshutkin-like reaction between ammonia and (S)-1,4-andydro-2,3-dideoxy-5-O-mesylpentitol (2a)
Fig. 1
Fig. 1
Structures of mesylate derivatives converted into ammonium salts
Scheme 1
Scheme 1
Reactions of ammonium salt formation
Fig. 2
Fig. 2
Rotamers exhibiting possible spatial arrangements of the OCH3 group in relation to the heterocyclic oxygen atom. The preferred orientation is in the box
Fig. 3
Fig. 3
Energy (E 0) and pseudochemical potential (U 0) profiles for reactions 14 calculated at B3LYP/6-31+G** level in the gas phase, chloroform and water
Fig. 4
Fig. 4
Definition of the endocyclic torsion angles ϕ 0ϕ 4
Fig. 5
Fig. 5
Geometries of the stationary points and ΔE (kcal mol−1) computed at the B3LYP/6-31+G** level for reactions 1 and 2 in the gas phase. Selected distances in Å, and valence angles in degrees
Fig. 6
Fig. 6
Geometries of the stationary points and ΔE (kcal mol−1) computed at the B3LYP/6-31+G** level for reactions 3 and 4 in the gas phase. Selected distances in Å, and valence angles in degrees
Fig. 7
Fig. 7
Comparison of activation barriers for reactions 1 and 2 with different nucleophiles in the gas phase
Fig. 8
Fig. 8
Geometry of the ion pair in reaction 1
Fig. 9
Fig. 9
Geometries of the transition states optimized at the B3LYP/6-31+G** level in water. Selected distances in Å, and valence angles in degrees

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