TY - JOUR
T1 - Kinetics of the phenyl radical reaction with ethylene
T2 - An RRKM theoretical analysis of low and high temperature data
AU - Yu, T.
AU - Lin, Ming-Chang
PY - 1995/1/1
Y1 - 1995/1/1
N2 - The kinetics of the reaction of phenyl radical with ethylene has been investigated with the cavity-ring-down method at six temperatures between 297 and 523 K under a constant pressure of 20 torr Ar. A test performed at 60-torr pressure revealed no noticeable change in the measured rate constant value. The second-order rate constant determined by directly monitoring the decay of the phenyl radical under excess ethylene concentration conditions could be effectively represented by the Arrhenius equation k"C2H4
= 10- 11.92± 0.35 exp (-2,250 ± 630/T) cm3/s where the errors represent one-standard deviation evaluated with the weighting factor wi = ( ki σi)2. This low-temperature and comparatively high-pressure result can be satisfactorily correlated by means of the RRKM theory with the high-temperature (1000-1300 K) and low-pressure (1-10 mtorr) styrene formation data reported by Fahr and Stein (Ref. 15), k″C6H5C2H3
= 4.2 × 10-12exp(-3120/T)cm3/s. The result of our multichannel RRKM calculation based on the mechanism C6H5 + C2H4 a ⇌ C6H5CH2CH2 b → C6H5C2H3 + H c → C6H5C2H4 +(M) suggests that the rate constant for the production of styrene under the conditions employed by Fahr and Stein (kb) is essentially the same as the total rate constant, k″C2H4
= kb + kc, because kb ≫ kc at high temperatures (T > 1000 K) and low pressures (P < 20 torr). Under atmospheric combustion conditions, however, both kb and kc are comparable and strongly dependent on T and P. The total rate constant for the C6H5 + C2H4 reaction can be given by the following expression: k"C2H4
= 1.2×10- 17 T 1.62 exp (-1490/T) cm3/s for the temperature range 300-2000 K, effectively encompassing both sets of kinetic data.
AB - The kinetics of the reaction of phenyl radical with ethylene has been investigated with the cavity-ring-down method at six temperatures between 297 and 523 K under a constant pressure of 20 torr Ar. A test performed at 60-torr pressure revealed no noticeable change in the measured rate constant value. The second-order rate constant determined by directly monitoring the decay of the phenyl radical under excess ethylene concentration conditions could be effectively represented by the Arrhenius equation k"C2H4
= 10- 11.92± 0.35 exp (-2,250 ± 630/T) cm3/s where the errors represent one-standard deviation evaluated with the weighting factor wi = ( ki σi)2. This low-temperature and comparatively high-pressure result can be satisfactorily correlated by means of the RRKM theory with the high-temperature (1000-1300 K) and low-pressure (1-10 mtorr) styrene formation data reported by Fahr and Stein (Ref. 15), k″C6H5C2H3
= 4.2 × 10-12exp(-3120/T)cm3/s. The result of our multichannel RRKM calculation based on the mechanism C6H5 + C2H4 a ⇌ C6H5CH2CH2 b → C6H5C2H3 + H c → C6H5C2H4 +(M) suggests that the rate constant for the production of styrene under the conditions employed by Fahr and Stein (kb) is essentially the same as the total rate constant, k″C2H4
= kb + kc, because kb ≫ kc at high temperatures (T > 1000 K) and low pressures (P < 20 torr). Under atmospheric combustion conditions, however, both kb and kc are comparable and strongly dependent on T and P. The total rate constant for the C6H5 + C2H4 reaction can be given by the following expression: k"C2H4
= 1.2×10- 17 T 1.62 exp (-1490/T) cm3/s for the temperature range 300-2000 K, effectively encompassing both sets of kinetic data.
UR - http://www.scopus.com/inward/record.url?scp=0028820982&partnerID=8YFLogxK
U2 - 10.1016/0010-2180(94)00085-7
DO - 10.1016/0010-2180(94)00085-7
M3 - Article
AN - SCOPUS:0028820982
SN - 0010-2180
VL - 100
SP - 169
EP - 176
JO - Combustion and Flame
JF - Combustion and Flame
IS - 1-2
ER -