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Thermal ignition of acetonitrile. Experimental results and kinetic modeling

✍ Scribed by Assa Lifshitz; Carmen Tamburu; Harvey F. Carroll


Publisher
John Wiley and Sons
Year
1997
Tongue
English
Weight
247 KB
Volume
29
Category
Article
ISSN
0538-8066

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✦ Synopsis


Ignition delay times of acetonitrile (CH 3 CN) in mixtures containing acetonitrile and oxygen diluted in argon were studied behind reflected shock waves. The temperature range covered was at overall concentrations behind the reflected shock wave ranging 1420-1750 K from 2 to mol/cm 3 . Over this temperature and concentration range the ignition delay Οͺ5 4 Ο« 10 times varied by approximately one order of magnitude, ranging from ca. 100 s to slightly above 1 ms. From a total of some 70 tests the following correlation for the ignition delay times was derived: s, Οͺ12 3 0.12 Οͺ0.76 0.34 t Ο­ 9.77 Ο« 10 exp(41.7 Ο« 10 /RT) Ο« {[CH CN] [O ] [Ar] } ign 3 2

where concentrations are expressed in units of mol/cm 3 and R is expressed in units of cal/(K mol). The ignition delay times were modeled by a reaction scheme containing 36 species and 111 elementary reactions. Good agreement between measured and calculated ignition delay times was obtained. A least-squares analysis of 60 computed ignition delay times from six different groups of initial conditions gave the following temperature and concentration dependence: and The ignition 3 E Ο­ 46.2 Ο« 10 cal/mol, ␀ Ο­ 0.43, ␀ Ο­ Οͺ1.18, ␀ Ο­ 0.18.

CH CN O Ar

3 2 process is initiated by H-atom ejection from acetonitrile. The addition of oxygen atoms to the system from the dissociation of molecular oxygen and from the reaction CH CN Ο© O : 3 2 is negligible. In view of the relatively high concentration of methyl radicals HO D Ο© CH CND 2 2 obtained in the reaction the branching step CH CN Ο© H : CH Ο© HCN, CH Ο© O : 3 3 3 2 plays a more important role than the parallel step A discussion CH O Ο© O H Ο© O : OH Ο© O. 3 2

of the mechanism in view of the sensitivity analysis is presented.


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