Direct transfer of aliphatic and aromatic substituents from organosilatranes to mercury(II) species

The relative reaction rates of several silatranes (derivatives of 2,8.9-trioxa-5-aza- 1-silatricyclo[3.3.3.0^1,5]undecane) and HgCl₂ in acetone-d₆to yield the corresponding organomercury compound are of the order of e.g., 5 × 10^?1 1 mol^?1 sec^?1 or slightly less, a rate that is unexpectedly high compared to the essentially inert parent organotrialkoxysilanes. Thus, the apical Si&.zsbnd;C bond of the silatrane is extraordinarily susceptible to direct electrophilic attack by mercury(II). The rates decrease in the order CH₂CH, C₆H₅, p-ClC₆H₄ > CH₃ > CH₃CH₂, CH₃CH₂CH₂ > C₆H₁₁, ClCH₂, Cl₂CH, CH₃CH₂O. The effects of varying the solvent and the counterions are noted, and the probable mechanism is discussed.     

Nuclear magnetic resonance study of selected derivatives of 2,8,9-trioxa-5-aza-1-silatricyclo[3.3.3.01,5]undecane (silatrane)

The ¹H, ¹³C and ²⁹Si nuclear magnetic resonance spectra of the parent compound and twelve derivatives of 2,8,9-trioxa-5-aza-1-silatricyclo[3.3.3.0^1,5]undecane (silatrane) are discussed. Effective Taft polarity constants for the silatrane substituents are proposed. An equation is developed to correlate the ²⁹Si NMR chemical shifts of the silatranes with the corresponding organo-triethoxysilanes.     

Gas‐phase geometries and energies of bis(2,2′‐bipyridine) interacting either with Cu(I) or Ag(I): Computational study

With a polarized double‐zeta basis set, we carried out MP2 and density functional theory geometry optimization of bis(2,2′‐bipyridine) interacting either with Cu(I) or Ag(I). The computed gas‐phase geometries of both Cu and Ag complexes present tetrahedral distortions around the ions. However, geometry optimization on Cu or Ag ions complexing with ammonia molecules yield perfect tetrahedral coordination and interaction energies comparable to those of the bis(2,2′‐bipyridine) complexes. Solid‐state laboratory studies on complexes of the same metal ions with substituted bis(2,2′‐bipyridine) revealed tetrahedral distortions around the ions, even stronger than those computed in the gas phase. From our analysis of the potential interaction energies we conclude that the origin of the larger distortions in the solid state result from stacking interactions. © 2003 Wiley Periodicals, Inc. Int J Quantum Chem 93: 395–404, 2003     

Divergent sequential reactions of β-(2-aminophenyl)-α,β-ynones with nitrogen nucleophiles

β-(2-Aminophenyl)-α,β-ynones readily react with nitrogen nucleophiles to give three major types of products, depending on reaction conditions and variation in the nucleophiles. The reaction may lead to simple 1,2-nucleophilic adducts or, at higher temperatures, to a divergent sequential cyclisation giving rise to 2-aryl-4-aminoquinolines by reaction with amines, or to substituted 2-aryl or 2-alkyl-4-alkylidene quinazolines by reaction with amidines. The latter could also be synthesised by reaction of β-(2-aminophenyl)-α,β-ynones with iminochlorides.     

Tautomeric equilibria of [1]benzopyrano[3,4-d]imidazol-4(3H)-ones, a theoretical and NMR study

[reaction: see text] Benzopyranoimidazolones could virtually exist in four tautomeric forms, namely N3-H, N1-H, coumarin O-H, and C2-H. Experimental evidence reported thus far has been unable to lead to a unique statement about the preferred tautomeric forms in solution. In this work, tautomeric equilibria for a series of 2-substituted [1]benzopyrano[3,4-d]imidazol-4(3H)-ones were investigated by DFT calculations, in both gas phase and solution. The influence of the solvent was included in the calculations by the CPCM solvent model. 13C chemical shifts of all tautomers were computed at different levels of theory and then compared with experiments to assign the preferred tautomers. Theoretical findings were then compared to dynamic 1H NMR experiments results.