Non-empirical calculations using the equations-of-motion approach are reported for iJ( 15Nt5N) in hydrazine, diazene, isodiazene, the azide anion, and nitrogen. Irrespective of the single or multiple nature of the bond between the nitrogens, iJ( isNi5N) should be negative in all compounds. The only
Theoretical study of the 1J(13C13C) indirect nuclear spin-spin coupling constant of the bridgehead bond in [1.1.1]propellane and related systems
โ Scribed by V. Galasso
- Publisher
- Elsevier Science
- Year
- 1994
- Tongue
- English
- Weight
- 350 KB
- Volume
- 230
- Category
- Article
- ISSN
- 0009-2614
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โฆ Synopsis
Ab initio calculations using the equations of motion approach are reported for 'J( 13C"C) of the bridgehead bond in [ 1.1.1 I-, 12.1.1 I-, [2.2.1 I-, [2.2.2]-, [3.2.1 ]-propellane, bicyclobutane, bicyclopentane, bicyclohexane and tetracyclopentane. The results give an overall picture of the influences exerted on sign and magnitude of 'J( 13C13C) by progressive condensation of the cyclobutane frame and by enlargement of the fused rings. Extraordinarily small values are predicted for [ 1.1.1 ]-propellane and [ 2.1.1 ]-propellane.
๐ SIMILAR VOLUMES
## Abstract The magnitude of the NMR spinโspin coupling constant, ^3^__J__(CH), between a vicinal ^13^Cโ^1^H pair depends, __inter alia__, on the value of the torsion angle ฮฆ~CH~(^13^C๏ฃฟC๏ฃฟC๏ฃฟH) and is influenced by the presence of an electronegative substituent located on the coupling ^13^C nucleus.
Theoretical calculations performed using the coupled Hartree-Fock perturbation theory (CHFPT) show that the MNDO approximation is superior to INDO and MIND03 in computing nuclear spin coupling constants between directly bonded carbon and hydrogen in polysubstituted methanes, HCXYZ. The CHFPT-MNDO pr