The kinetics of the elimination of hydrogen fluoride from chemically activated 1,1,2-trifluoroethane and 1,1,2,2-tetrafluoroethane
Abstract
The rates of elimination of hydrogen fluoride have been compared with rates of stabilisation by collision for chemically activated 1,1,2-trifluoroethane and 1,1,2,2-tetrafluoroethane molecules over a range of pressure and temperature. The energised molecules have been produced by radical combination from (a) photolysis of 1,1,3,3-tetrafluoroacetone and (b) co-photolysis of 1,3-difluoroacetone and 1,1,3,3-tetrafluoroacetone. The ratios of k(elimination of hydrogen fluoride)/k(deactivation by collision) at room temperature are 0·1 cm. (CH2F·CHF2) and 0·0015 cm. (CHF2·CHF2). The classical Rice–Ramsperger–Kassel theory of unimolecular reactions is shown to give a quantitative description of the decomposition of the energised molecules. Reasonable values of the activation energies for the hydrogen fluoride elimination reaction are CH2·CHF2= total C2H2F2+ HF 59 kcal. mole–1, =cis-CHF![[double bond, length half m-dash]](https://www.rsc.org/images/entities/char_e006.gif) CHF + HF 58 kcal. mole–1, =trans-CHF
CHF + HF 58 kcal. mole–1, =trans-CHF![[double bond, length half m-dash]](https://www.rsc.org/images/entities/char_e006.gif) CHF + HF 60–61 kcal. mole–1, = CH2
CHF + HF 60–61 kcal. mole–1, = CH2![[double bond, length half m-dash]](https://www.rsc.org/images/entities/char_e006.gif) CF2+ HF 59 kcal. mole–1, HF2·CHF2= CHF
CF2+ HF 59 kcal. mole–1, HF2·CHF2= CHF![[double bond, length half m-dash]](https://www.rsc.org/images/entities/char_e006.gif) CF2+ HF 63 kcal. mole–1
CF2+ HF 63 kcal. mole–1
 
                



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