Rate constants have been determined at (298 \* 4) K for the reactions: and the relaxation processes: (lb) HF(u = 1) + HCN -HF(v = 0) + HCN Time-resolved HF(1,O) emission was observed following the photolysis of Fz with pulses from an excimer laser operating on XeCl ( h = 308 nm). Analysis of the
Vibrational relaxation of HF(v = 1) by F atoms
β Scribed by Ronald L. Thommarson; George C. Berend
- Publisher
- John Wiley and Sons
- Year
- 1974
- Tongue
- English
- Weight
- 927 KB
- Volume
- 6
- Category
- Article
- ISSN
- 0538-8066
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β¦ Synopsis
Abstract
The rate of vibrational relaxation of HF(v = 1) by F atoms has been calculated using quasiβclassical trajectory techniques. An attempt has been made to account for the effects of multiple potential energy surfaces on the vibrational relaxation efficiency within the electronically adiabatic assumption. Toward this end two potential energy surfaces were investigated. The LEPS equation was used to construct a reactive surface for F + HFβ² β FH + Fβ² having a reaction barrier height of 5.4 kcal/mole, which is in agreement with a bond energyβbond order prediction. A nonreactive interaction potential consisting of atomβatom Morse functions was calibrated to Noble and Kortzeborn's [J. Chem. Phys. 52, 5375 (1970)] LCAOβMOβSCF results for FHF(^2^II). The results are in qualitative agreement with experiment. However, the nonreactive surface appears to be too repulsive, and consequently, the contribution of collisions on the nonreactive surface to the total vibrational relaxation rate coefficient are overestimated.
π SIMILAR VOLUMES
The laser induced fluorescence method has been used to measure the rate of deactivation of HF(u = 1) by F, 0, and H atoms at 300Β°K. The rate for F-atoms was found to be kF\_HF = (0.9 f 0.2) X lo4 set-' torr-', for Oatoms Lo\_m = (1.0 f 0.2) X lo5 set-' torr-', and for Hatoms, an upper limit to the r
The vibrational relasation time for COz(v3) + O(3P) has been mcasurcd by Inscr fluorescence. The observed value, pCo2,0 = 0.21 \* 0.04 fiscc, is an order of mqniludc lower than the relaxation time for self-collisions.
An ~b mhio. quxuum-nwch3nlrxl nwhod IS used IO compute rxc cocfiiicisnls ior the ubral~onsl rclau~l~on olozonc III ihrccdlmcnslonal colbslons WII~ bcbum atoms Good qxeemcnt 15 obr~mcd bctwccn tbr c.~lcul~tcd and qwmwlsl MC cocfiicwnts Tar the process Ilc -F @(OlO) -Ilc + 03(000)
The vibrational relaxation of HCl(u= 1) by chlorine and bromine atoms has been me:lsured at 295 K by :I discharge fbW SySti%l using the resonance fluorescence method to dctcct the hiIlogen atom concentration, combined with laser induced tkorescencc. T&c rnessured rate comtants arc: K(HCI-Cl) = (7.0