The Liu-Dykstra theory of electrical influence on vibrational potentials in hydrogen bonded complexes is shown to account very well for vibrational frequency shifts and induced dipoles in a series of rare gas complexes with hydrogen fluoride. The behavior of the electrical interaction energy and dip
OH bonds in electric fields: electron densities and vibrational frequency shifts
✍ Scribed by Kersti Hermansson
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 605 KB
- Volume
- 233
- Category
- Article
- ISSN
- 0009-2614
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✦ Synopsis
The changes in the electron density distribution caused by varying the O-H bond length for HDO and OH-in uniform electric fields are investigated and related to the frequency shifts for the uncoupled O-H stretching vibration. Numerical integration of difference density maps, Ap= p( roH + ArOH) -p( rOH), reproduces the electronic contribution to apii""I/ at-,, , if the integration is carried out to a distance of = 3.5 A from the 0 atom. The frequency shift A v is proportional to -E,, x [d/Ltp"="' (IoH) /dr&-&% VP iyduced( E,, , rOH) /&-OH] and electron density maps corresponding to the electronic parts of these terms are presented. Experimentally it has been found that the OH -ion shows a frequency upshift when bound in a moderately strong field, while water molecules show a downshift. The electron density maps show why dpr"'-"'( roH) /drOH is positive for HDO and negative for OH -, resulting in a downshift for bound water an an upshift for bound OH-. For positive fields, a~~;dUCedl aroH is positive for both HDO and OH -and gives a downshift contribution.
📜 SIMILAR VOLUMES
Proton nuclear magnctlc shxldmg tensors arc calculated for some O-H...0 hydrogen bonds. (H302); (HzO)z, and (H50~)+. The effects of charge, geometry. and bws set are stuled. Agreement ~7th single crystal p&cd NhlR evperimcnts is obtamcd. A Itneer dependence betwcn the proton chcmwal shift and the 0.
Infrx;ed SpCtiOScopic m?osurements in solution zt low temperatures show in the case of substituted phenols, thzr in kphase and on out-of-phase OH st-etching vibxtion exists due to the coupling oi vibrational motions of adjacent OK group ir! hq.&ogen bonded "golym~-rs".
## Abstract The ability to use calculated OH frequencies to assign experimentally observed peaks in hydrogen bonded systems hinges on the accuracy of the calculation. Here we test the ability of several commonly employed model chemistries—HF, MP2, and several density functionals paired with the 6‐3