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Deactivation of Vibrationally Excited Carbon Dioxide (ν3) by Collisions with Carbon Dioxide or with Nitrogen
178
Citations
11
References
1969
Year
Carbon DioxideEngineeringChemistryElectronic Excited StateLaser Fluorescence MethodChemical EngineeringMolecular KineticsExcited MoleculePhotophysical PropertyPhysicsPhysical ChemistryQuantum ChemistryExcited State PropertyCarbonizationLaser PhotochemistryNatural SciencesSpectroscopyChemical KineticsRate Constants
The rate constants associated with the deactivation of vibrationally excited CO2*(ν3) by collision with either CO2 or N2 have been experimentally determined from 300°–1000°K by a laser fluorescence method. The reactions investigated were CO2*(ν3)+N2⇆ lim k−5k5CO2+N2*, CO2*(ν3)+N2→ lim k5CO2*(ν1, ν2)+N2, CO2(ν3)+CO2→ lim k1CO2*(ν1, ν2)+CO2, N2*+CO2→ lim k7CO2*(ν1, ν2)+N2, where the asterisk denotes a vibrationally excited molecule, and the quantities in parentheses represent the specific excited modes of CO2. The rate constant k5 varies with temperature T (°K) as 8.60 × 107 / T3/2torr−1·sec−1. From 400°–1000°K the rate constant k1 (per torr−1 ·second−1) varies with temperature as log10k1 = A − BT−1 / 3 with A = 6.79 and B = 30.8. From 300°–400°K the measured values of k1 are greater than those corresponding to the above relation. The rate constant k6 increases from a value of 110 torr−1·sec−1 at room temperature to a value of 2700 torr−1·sec−1 at 1000°K, but the variation of k6 with temperature cannot be simply expressed. The rate constant k7 was found to be negligibly small compared to the other rate constants.
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