THERMAL DECOMPOSITONS OF 1,1,1-TRIFLUOROETHANE AND PENTAFLUOROETHANE IN A TURBULENT FLOW REACTOR
The thermal decompositions of 1,1,1-trifluoroethane (CH 3 CF 3 ) and pentafluoroethane (CHF 2 CF 3 ) were studied by using a turbulent flow reactor at atmospheric pressure over the temperature ranges of 1213-1333 K and 1273-1373 K. The rate coefficients for these thermal decompositions were determin...
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Veröffentlicht in: | Combustion science and technology 2007-06, Vol.179 (7), p.1417-1432 |
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Format: | Artikel |
Sprache: | eng |
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Zusammenfassung: | The thermal decompositions of 1,1,1-trifluoroethane (CH
3
CF
3
) and pentafluoroethane (CHF
2
CF
3
) were studied by using a turbulent flow reactor at atmospheric pressure over the temperature ranges of 1213-1333 K and 1273-1373 K. The rate coefficients for these thermal decompositions were determined from the first-order decays of the reactants to be k(CH
3
CF
3
) = 10
12.9±1.2
exp[−(276 ± 29) kJ ⋅ mol
−1
/RT] and k(CHF
2
CF
3
) = 10
13.9±1.4
exp [−(324 ± 36) kJ ⋅ mol
−1
/RT]s
−1
. To examine the reaction paths, we identified the decomposition products using gas chromatography-mass spectrometry (GC-MS) and performed ab initio MO calculations. These results showed that the sequential HF elimination reactions, CH
3
CF
3
→ CH
2
CF
2
+ HFand CH
2
CF
2
→ CHCF + HF, were favorable for the CH
3
CF
3
pyrolysis. On the other hand, four initial steps: CHF
2
CF
3
→ CF
3
CF + HF, CHF
2
CF
3
→ CF
2
CF
2
+ HF, CHF
2
CF
3
→ CHF
3
+ CF
2
and CHF
2
CF
3
→ CHF
2
+ CF
3
, were possible for the CHF
2
CF
3
pyrolysis. Such a difference in the reaction paths between the CH
3
CF
3
, and CHF
2
CF
3
pyrolyses can be explained by fluorine hyperconjugation and by repulsion between the fluorine atoms on the 1- and 2-carbons of each hydrofluoroethane. |
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ISSN: | 0010-2202 1563-521X |
DOI: | 10.1080/00102200601181962 |