The coeffkients which determine the electric field dependence of the mean proton shielding to second order in the field have been calculated by a finite field method at the SCF level for the binary hydrides CH4, NHs, HaO, HF, SiH4, PHs, HrS and HCl. The paramagnetic parts of the coefftcients are con
Electric field effects on the shielding of protons in CH bonds
β Scribed by Martin Grayson; William Thomas Raynes
- Publisher
- John Wiley and Sons
- Year
- 1995
- Tongue
- English
- Weight
- 609 KB
- Volume
- 33
- Category
- Article
- ISSN
- 0749-1581
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β¦ Synopsis
Abstract
The coefficients which determine the electric field dependence at first and second order of the shielding of protons in Cο£ΏH bonds were calculated by a finiteβfield SCF method for the molecules, CH~4~, C~2~H~6~, CH~3~F, CH~3~Cl, CH~3~CN, C~2~H~4~, H~2~CO, HCN and C~2~H~2~. Values are given for individual tensor components and for the rotationally averaged coefficients. Diamagnetic and paramagnetic parts of the coefficients are generally of the same order of magnitude. This differs from carbon, nitrogen, oxygen and fluorine shielding studied previously where the paramagnetic parts are often very much larger than their diamagnetic counterparts. The linear electric field coefficients A~z~ (electric field along the Cο£ΏH bond from C to H) for the above molecules (except H~2~CO and HCN) are very similar in value, with a mean of 70.0 ppm a.u. This is very close to an empirical value of 72.2 ppm a.u. obtained by ZΓΌrcher in a classic study of steroids. It further appears that the value may be transferable among all C(sp^3^)ο£ΏH bonds. A representative value for the mean quadratic coefficient B is 68.0 ppm a.u. Empirical values of this vary widely.
π SIMILAR VOLUMES
A column headed o= was inadvertently omitted from Table 1. The numbers in this column which differ from zero are as follows: -1.17 for NH3, -1.01 for H20, -0.72 for PH3 and -2.00 for H2S. The value ofox~ for H2S in Table 1 should be -1.00 (not -1.04). In the final paragraph of the Letter the numeri
The changes in the components of the nuclear shielding tensors which occur when a molecule is placed in a uniform electric field can be described by a Taylor series expansion. The coefficients in this expansion are sometimes referred to as "shielding polarizabilities". Following a study of electric
## Abstract The optimized geometry of isolated trimethylamine (TMA), its hydrogen bond complexes with phenol derivatives and protonated TMA is calculated at the B3LYP/6β31++G(d,p) level. A natural bond orbital (NBO) analysis on these systems is carried out at the same level of theory. In isolated T
We discuss the effects of the electric field present in the STM on the frequency and spatial localization of (vibrational) excitations induced by inelastic electron tunneling. We show that, depending on its direction and size, the field can produce either a weakening or a strengthening of chemical b